Number of wireless sensors needed to detect a wildfire

Size: px
Start display at page:

Download "Number of wireless sensors needed to detect a wildfire"

Transcription

1 Number of wireless sensors neee to etect a wilfire Pablo I. Fierens Instituto Tecnológico e Buenos Aires (ITBA) Physics an Mathematics Department Av. Maero 399, Buenos Aires, (C1106ACD) Argentina pfierens@itba.eu.ar Abstract The lack of extensive research in the application of inexpensive wireless sensor noes for the early etection of wilfires motivate us to investigate the cost of such a network. As a first step, in this paper we present several results which relate the time to etection an the burne area to the number of sensor noes in the region which is protecte. We prove that the probability istribution of the burne area at the moment of etection is approximately exponential, given that some hypotheses hol: the positions of the sensor noes are inepenent ranom variables uniformly istribute an the number of sensor noes is large. This conclusion epens neither on the number of ignition points nor on the propagation moel of the fire. Page 1

2 1 Introuction The well-establishe literature on wireless sensor networks continuously mentions prevention an early etection of wilfires as a typical application of the fiel. However, to the best of our knowlege, only a few proposals of inexpensive sensor networks have been actually mae in the literature (e.g., Roriguez et al. (000); Yu et al. (005)) an only one has been implemente an trie to a small scale (Chen et al. (003); Doolin et al. (004); Glaser (004); Doolin an Sitara (005)). The lack of actual experiences on the implementation of wireless sensor networks for the etection of wilfires an the current problematic of forest fires in Argentina lea a group of researchers at ITBA to become involve in a mi-term project for the evelopment of such a network. As part of the project, forestry companies were consulte about their nees an experiences on fire etection. Companies in the region use mainly two alternative ways of fire etection (private communication). On one han, the most extene practice is the visual inspection of large areas (with a coverage raius of up to 0 km) from high towers an the aily walk of personnel through pre-establishe paths uring the fire-season. This type of system is very cheap because its main cost is represente by the low wages of the few people involve in the irect observation. On the other han, a few companies have also implemente the observation through cameras in the visual an infrare ranges. However, this class of system is usually consiere too expensive because the relatively high initial cost of installation of the infrare cameras. Uner this situation, several companies were intereste in the iea of a wireless sensor network for the etection of wilfires, but they were also concerne on the cost of the system per unit of area. This problem can be ecompose mainly into two parts: a) the cost Page

3 of each iniviual noe; b) the number of noes which are neee per unit of area (i.e., the number of noes per square meter). In this paper we investigate part b), while part a) will be presente elsewhere. 1.1 Variables uner analysis We shall work with simple two imensional moels an we shall eal only with propagation of surface fires. Moreover, we shall keep the moel of the wireless sensors as simple as possible, that is, we shall assume that all sensors allow for the etection of the fire as soon as the fire reaches their location. Finally, we shall not concern ourselves with the ifficulties of the communication among the sensors, which may be impaire by the activity of the fire itself (Heron an Mphale (004), Mphale et al. (007)). Uner this setting, there are many variables relate to the number of wireless sensors that can be stuie. We choose to of them, the time to etection (T ) an the area alreay burnt at the time of the etection (A ). Both variables can be relate, in turn, to the resources neee for contention of the fire after it has been etecte. Since the number of wireless sensors may vary accoring to the extension of the region that must be protecte, we shall use the characteristic istance between sensors (D) as reference inepenent of the actual area. Although the efinition of the characteristic istance between sensors may vary slightly from one setting to another, in all cases it subsumes uner a single value how wiely space the sensors are. The rest of the paper is structure as follows. In Section, we present some simple results for the case where the noes are istribute in a regular pattern across the area of interest. In Section 3, we analyze the expecte time to etection an the burne area before Page 3

4 etection when the sensor noes are ranomly istribute in the protecte area. Section 4 summarizes the main conclusions of the paper an mentions some ieas for future work. Regularly istribute sensors In this section, we analyze the case where the sensors are locate in a regular gri in such a way that the istance between any pair of them in the same row or the same column is D, the characteristic istance in this setting. As a further simplification, we shall assume that the region to be protecte is a rectangle whose sies are integer multiples of D. It is easy to exten the work in this section to more general regions by partitioning them into small rectangular pieces..1 Circular propagation at constant rate We assume that surface fires propagate at a constant rate of sprea (R) in all irections an that the probability of ignition is uniformly istribute insie the protecte area. Both the uniform istribution of the probability of ignition an the fact that the noes are locate in a regular lattice enable us to reuce the stuy of the etection of a fire to a much smaller area corresponing to a square elimite by four sensor noes, one on each vertex. Furthermore, this square can be split up into four smaller squares, as shown in Figure 1. Given the assumption that a fire propagates in all irections at the same spee, if a fire originates in Region i (i =1,, 3, 4 see Figure 1), it will be etecte by sensor i first. Therefore, we can further limit our analysis to only one of the four regions an the corresponing noe, say, Region 1 an sensor noe 1. In other wors, P ( T x) = P[ T x the fire originate in Region 1]. Page 4

5 Notice that T is simply the istance from the ignition point to the sensor noe ivie by the constant rate of sprea R. Since the istribution of the ignition point is uniform insie Region 1, we have [ T x the fire originate in Region 1]= P [ Distance from sensor 1 to the ignition point Rx the fire originate in Region ] = = P 1 Area of the surface whose points are at a istance Rx of sensor 1 = Area of Region 1 After some work, the latter expression can be foun to be π Rx P( T x) si Rx D =, 4 D (1) π 1 ( ) tan Rx 1 Rx Rx P T + x = 1 si D D, 4 Rx () D D D ( T x) = 1 si Rx D. P (3) Further algebraic work leas to D π P T = , (4) R 4 + log [ ] ( 1+ ) D D E T = 0.386, (5) 6 R R E 1 D 6 [ ] ( ) ( + log( 1+ ) D D T =, var T = 0.003, (6) 6 R 36 R R π E[ A ] = D 0.5 D. (7) 6. Page 5

6 Some comments are ue. Equation (4) points out that more than 80% of fires will be etecte in less than D/R an, hence, their area will be smaller than πd /4. Equation (5) says that, as expecte, the mean etection time is proportional to the ratio D/R. Finally, while Equations (1)-(3) imply that no fire will have an area greater than πd / at the moment of etection, Equation (7) says that the expecte value of such area is approximately D /. In particular, note that the expecte value of the area of the fire at the moment of etection oes not epen on the rate of sprea of the fire, but it only epens on the characteristic istance D. 3 Ranomly istribute sensors In this section, we analyze the case where the sensors are ranomly istribute in the region to be protecte. In this case, the characteristic istance D is the mean istance between sensors compute as A D =, (14) N where A is the total area of the protecte region an N is the total number of sensors. We shall first show that, when the number of sensors is large, the burne area at the moment of etection A has a simple probability istribution which is inepenent of the propagation moel. We shall then show simple approximations for the statistics of the time to etection for simple propagation moels. 3.1 Probability istribution of the burne area The probability that the burne area A is greater than a given number x is equal to the probability that the fire has not foun any sensor insie the burne region. Since sensor Page 6

7 noes are ranomly istribute across the protecte region, an assuming that the position of each sensor is inepenent of that of the others, we have P ( A > x) = 1, where A is the total area of the protecte region an N is the total number of sensor noes. Using Equation (14), we can write Note that, as N, P P x A ( A > x) = 1 = 1. x D N x ND N N N x D N ( A x) = exp. N x D > 1 N Formally, we have the following Theorem 1. Assume the locations of sensor noes are inepenent an ientically istribute ranom variables with uniform istribution across the protecte region. Furthermore, assume that the position of the sensor noes an the ignition points (there may be more than one) are inepenent ranom variables. Let N be the number of sensor noes an A(N) the surface area of the protecte region, which varies with N in such a way that A(N) = D N, where D is a positive constant. Then, as the number N of sensor noes goes to infinity, the ranom variable A corresponing to the burne area at the moment of etection converges in istribution to an exponential ranom variable with parameter λ=1/d. Page 7

8 Probably, the most salient feature of Theorem 1 is that it oes not epen on the propagation law of the fire an it epens neither on the number nor on the istribution of the ignition points. In other wors, Theorem 1 states that, if the protecte area is large an the number of sensor noes is also large, then P x D ( A > x) exp, E[ A ] D, var( A ). D 3. Probability istribution of the time to etection Theorem 1 leas to the following simple Corollary 1. Assume that there is a eterministic law F such that, at each time instant t, F(t) represents the total burne area at time t. If the hypotheses of Theorem 1 are satisfie, then, as the number of sensor noes N goes to infinity, P F( t) exp D ( T t). > N In the following paragraphs, we consier two simple examples of application of Corollary Circular propagation at constant rate Note that, as the surface area of the protecte region increases, we may ignore the cases where the fire evelops near the borers of the region. Then, it is easy to see that the function F in Corollary 1 for the case of circular propagation at constant rate of sprea R is given by F ( t) = π ( Rt). Page 8

9 Then, for a large area covere with a large number of sensors, we can make the following approximation: πr t exp D ( T > t). P So we can estimate the expecte value of the time to etection as E πr t D = R 0 0 D [ T ] P( T > t) t exp t, = where we have omitte the etails of the calculation. In a similar fashion, we get E D 4 π D D [ T ] var( T ) πr, Figures an 3 show the agreement of the previous equations an the results of simulations (10 5 Monte Carlo runs) with D=1 m, R=1 m/s, N varying from 10 to an one ranom ignition point. 4π R R 3.. Elliptical propagation at constant rate In this section, we consier the case of a surface fire that propagates with an elliptical shape an at a constant rate of sprea. In this case, the function F is given by (see Finney (1998)) F HB 4LB ( t) = π R t, where R is the rate of sprea, HB is the Hea-to-Back ratio an LB is the Length-to-Breath ratio. In a similar fashion as before, we can compute Page 9

10 LB D [ T ], E[ T ] 4LB D E, 1 R 1 1 πr + HB 1 + HB var 4 π 4LB D 4LB D ( T ) π 1 R 1 R HB HB 4 Conclusions The lack of extensive research in the application of inexpensive wireless sensor noes for the early etection of wilfires motivate us to investigate the cost of such a network. As a first step, in this paper we present several results which relate the time to etection an the burne area to the number of sensor noes in the region which is protecte. Our main result is Theorem 1 which states that the probability istribution of the burne area is approximately exponential, given that some hypotheses hol: the positions of the sensor noes are inepenent ranom variables uniformly istribute an the number of sensor noes is large. It is important to remark that this conclusion epens neither on the propagation moel of the fire nor on the number an istribution of ignition points. Our next step in the investigation of the cost of a network of sensor noes for the etection of wilfires is to actually buil prototypes of such noes an to test their behavior uner controlle fires. Acknowlegements This work was partially supporte by anonymous contributors through the project Prevention an early etection of forest fires by means of sensor networks which is being evelope at the Instituto Tecnológico e Buenos Aires (ITBA). Page 10

11 References Chen MM, Majii C, Doolin DM, Glaser SD, Sitar N (003) Design an construction of a wilfire instrumentation system using networke sensors. Presente in Network Embee Systems Technology (NEST) Retreat 003. (Oaklan, California) Doolin DM, Glaser SD, Sitar N (004) Software Architecture for GPS-enable Wilfire Sensorboar. Presente in TinyOS Technology Exchange, February 6, 004. (University of California: Berkeley, California) Doolin DM, Sitara N (005) Wireless sensors for wilfire monitoring. In Proceeings of SPIE Symposium on Smart Structures & Materials, SPIE 5765, Finney MA (1998) FARSITE: Fire Area Simulator-Moel evelopment an evaluation. USDA Forest Service, Rocky Mountain Research Station Research Paper RMRS-RP-4. (Ogen, UT) Glaser SD (004) Some real-worl applications of wireless sensor noes. In Proceeings of SPIE Symposium on Smart Structures & Materials, SPIE 5391, Heron ML, Mphale K (004) Raio Wave Attenuation in Bushfires, Tropical Cyclones an Other Severe Atmospheric Conitions. Final Report on EMA Project 60/001. (School of Mathematical an Physical Sciences, James Cook University: Australia) Page 11

12 Mphale K, Heron M, Verma T (007) Effect of Wilfire-Inuce Thermal Bubble on Raio Communication. Progress In Electromagnetics Research 68, Roriguez N, Bistue G, E. Hernanez, Egurrola D (000) GSM front-en to forest fire etection. In Proceeings of the IEEE International Symposium on Technology an Society 000: University as a Brige from Technology to Society, Yu L, Wang N, Meng X (005) Real-time Forest Fire Detection with Wireless Sensor Networks. In Proceeings of the International Conference on Wireless Communications, Networking an Mobile Computing 005,, Page 1

13 Figure 1 Page 13

14 Figure Page 14

15 Figure 3 Page 15

Chapter 6: Energy-Momentum Tensors

Chapter 6: Energy-Momentum Tensors 49 Chapter 6: Energy-Momentum Tensors This chapter outlines the general theory of energy an momentum conservation in terms of energy-momentum tensors, then applies these ieas to the case of Bohm's moel.

More information

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012 CS-6 Theory Gems November 8, 0 Lecture Lecturer: Alesaner Mąry Scribes: Alhussein Fawzi, Dorina Thanou Introuction Toay, we will briefly iscuss an important technique in probability theory measure concentration

More information

Time-of-Arrival Estimation in Non-Line-Of-Sight Environments

Time-of-Arrival Estimation in Non-Line-Of-Sight Environments 2 Conference on Information Sciences an Systems, The Johns Hopkins University, March 2, 2 Time-of-Arrival Estimation in Non-Line-Of-Sight Environments Sinan Gezici, Hisashi Kobayashi an H. Vincent Poor

More information

A note on asymptotic formulae for one-dimensional network flow problems Carlos F. Daganzo and Karen R. Smilowitz

A note on asymptotic formulae for one-dimensional network flow problems Carlos F. Daganzo and Karen R. Smilowitz A note on asymptotic formulae for one-imensional network flow problems Carlos F. Daganzo an Karen R. Smilowitz (to appear in Annals of Operations Research) Abstract This note evelops asymptotic formulae

More information

Thermal conductivity of graded composites: Numerical simulations and an effective medium approximation

Thermal conductivity of graded composites: Numerical simulations and an effective medium approximation JOURNAL OF MATERIALS SCIENCE 34 (999)5497 5503 Thermal conuctivity of grae composites: Numerical simulations an an effective meium approximation P. M. HUI Department of Physics, The Chinese University

More information

05 The Continuum Limit and the Wave Equation

05 The Continuum Limit and the Wave Equation Utah State University DigitalCommons@USU Founations of Wave Phenomena Physics, Department of 1-1-2004 05 The Continuum Limit an the Wave Equation Charles G. Torre Department of Physics, Utah State University,

More information

The total derivative. Chapter Lagrangian and Eulerian approaches

The total derivative. Chapter Lagrangian and Eulerian approaches Chapter 5 The total erivative 51 Lagrangian an Eulerian approaches The representation of a flui through scalar or vector fiels means that each physical quantity uner consieration is escribe as a function

More information

Lower Bounds for the Smoothed Number of Pareto optimal Solutions

Lower Bounds for the Smoothed Number of Pareto optimal Solutions Lower Bouns for the Smoothe Number of Pareto optimal Solutions Tobias Brunsch an Heiko Röglin Department of Computer Science, University of Bonn, Germany brunsch@cs.uni-bonn.e, heiko@roeglin.org Abstract.

More information

Least-Squares Regression on Sparse Spaces

Least-Squares Regression on Sparse Spaces Least-Squares Regression on Sparse Spaces Yuri Grinberg, Mahi Milani Far, Joelle Pineau School of Computer Science McGill University Montreal, Canaa {ygrinb,mmilan1,jpineau}@cs.mcgill.ca 1 Introuction

More information

On colour-blind distinguishing colour pallets in regular graphs

On colour-blind distinguishing colour pallets in regular graphs J Comb Optim (2014 28:348 357 DOI 10.1007/s10878-012-9556-x On colour-blin istinguishing colour pallets in regular graphs Jakub Przybyło Publishe online: 25 October 2012 The Author(s 2012. This article

More information

3-D FEM Modeling of fiber/matrix interface debonding in UD composites including surface effects

3-D FEM Modeling of fiber/matrix interface debonding in UD composites including surface effects IOP Conference Series: Materials Science an Engineering 3-D FEM Moeling of fiber/matrix interface eboning in UD composites incluing surface effects To cite this article: A Pupurs an J Varna 2012 IOP Conf.

More information

What s in an Attribute? Consequences for the Least Common Subsumer

What s in an Attribute? Consequences for the Least Common Subsumer What s in an Attribute? Consequences for the Least Common Subsumer Ralf Küsters LuFG Theoretical Computer Science RWTH Aachen Ahornstraße 55 52074 Aachen Germany kuesters@informatik.rwth-aachen.e Alex

More information

Sharp Thresholds. Zachary Hamaker. March 15, 2010

Sharp Thresholds. Zachary Hamaker. March 15, 2010 Sharp Threshols Zachary Hamaker March 15, 2010 Abstract The Kolmogorov Zero-One law states that for tail events on infinite-imensional probability spaces, the probability must be either zero or one. Behavior

More information

Expected Value of Partial Perfect Information

Expected Value of Partial Perfect Information Expecte Value of Partial Perfect Information Mike Giles 1, Takashi Goa 2, Howar Thom 3 Wei Fang 1, Zhenru Wang 1 1 Mathematical Institute, University of Oxfor 2 School of Engineering, University of Tokyo

More information

ensembles When working with density operators, we can use this connection to define a generalized Bloch vector: v x Tr x, v y Tr y

ensembles When working with density operators, we can use this connection to define a generalized Bloch vector: v x Tr x, v y Tr y Ph195a lecture notes, 1/3/01 Density operators for spin- 1 ensembles So far in our iscussion of spin- 1 systems, we have restricte our attention to the case of pure states an Hamiltonian evolution. Toay

More information

6. Friction and viscosity in gasses

6. Friction and viscosity in gasses IR2 6. Friction an viscosity in gasses 6.1 Introuction Similar to fluis, also for laminar flowing gases Newtons s friction law hols true (see experiment IR1). Using Newton s law the viscosity of air uner

More information

arxiv: v2 [cond-mat.stat-mech] 11 Nov 2016

arxiv: v2 [cond-mat.stat-mech] 11 Nov 2016 Noname manuscript No. (will be inserte by the eitor) Scaling properties of the number of ranom sequential asorption iterations neee to generate saturate ranom packing arxiv:607.06668v2 [con-mat.stat-mech]

More information

Quantum Mechanics in Three Dimensions

Quantum Mechanics in Three Dimensions Physics 342 Lecture 20 Quantum Mechanics in Three Dimensions Lecture 20 Physics 342 Quantum Mechanics I Monay, March 24th, 2008 We begin our spherical solutions with the simplest possible case zero potential.

More information

APPROXIMATE SOLUTION FOR TRANSIENT HEAT TRANSFER IN STATIC TURBULENT HE II. B. Baudouy. CEA/Saclay, DSM/DAPNIA/STCM Gif-sur-Yvette Cedex, France

APPROXIMATE SOLUTION FOR TRANSIENT HEAT TRANSFER IN STATIC TURBULENT HE II. B. Baudouy. CEA/Saclay, DSM/DAPNIA/STCM Gif-sur-Yvette Cedex, France APPROXIMAE SOLUION FOR RANSIEN HEA RANSFER IN SAIC URBULEN HE II B. Bauouy CEA/Saclay, DSM/DAPNIA/SCM 91191 Gif-sur-Yvette Ceex, France ABSRAC Analytical solution in one imension of the heat iffusion equation

More information

Convergence of Random Walks

Convergence of Random Walks Chapter 16 Convergence of Ranom Walks This lecture examines the convergence of ranom walks to the Wiener process. This is very important both physically an statistically, an illustrates the utility of

More information

Analysis on a Localized Pruning Method for Connected Dominating Sets

Analysis on a Localized Pruning Method for Connected Dominating Sets JOURNAL OF INFORMATION SCIENCE AND ENGINEERING 23, 1073-1086 (2007) Analysis on a Localize Pruning Metho for Connecte Dominating Sets JOHN SUM 1, JIE WU 2 AND KEVIN HO 3 1 Department of Information Management

More information

Chromatic number for a generalization of Cartesian product graphs

Chromatic number for a generalization of Cartesian product graphs Chromatic number for a generalization of Cartesian prouct graphs Daniel Král Douglas B. West Abstract Let G be a class of graphs. The -fol gri over G, enote G, is the family of graphs obtaine from -imensional

More information

12.11 Laplace s Equation in Cylindrical and

12.11 Laplace s Equation in Cylindrical and SEC. 2. Laplace s Equation in Cylinrical an Spherical Coorinates. Potential 593 2. Laplace s Equation in Cylinrical an Spherical Coorinates. Potential One of the most important PDEs in physics an engineering

More information

Chapter 4. Electrostatics of Macroscopic Media

Chapter 4. Electrostatics of Macroscopic Media Chapter 4. Electrostatics of Macroscopic Meia 4.1 Multipole Expansion Approximate potentials at large istances 3 x' x' (x') x x' x x Fig 4.1 We consier the potential in the far-fiel region (see Fig. 4.1

More information

Quantum mechanical approaches to the virial

Quantum mechanical approaches to the virial Quantum mechanical approaches to the virial S.LeBohec Department of Physics an Astronomy, University of Utah, Salt Lae City, UT 84112, USA Date: June 30 th 2015 In this note, we approach the virial from

More information

A Review of Multiple Try MCMC algorithms for Signal Processing

A Review of Multiple Try MCMC algorithms for Signal Processing A Review of Multiple Try MCMC algorithms for Signal Processing Luca Martino Image Processing Lab., Universitat e València (Spain) Universia Carlos III e Mari, Leganes (Spain) Abstract Many applications

More information

Delay Limited Capacity of Ad hoc Networks: Asymptotically Optimal Transmission and Relaying Strategy

Delay Limited Capacity of Ad hoc Networks: Asymptotically Optimal Transmission and Relaying Strategy Delay Limite Capacity of A hoc Networks: Asymptotically Optimal Transmission an Relaying Strategy Eugene Perevalov Lehigh University Bethlehem, PA 85 Email: eup2@lehigh.eu Rick Blum Lehigh University Bethlehem,

More information

Transmission Line Matrix (TLM) network analogues of reversible trapping processes Part B: scaling and consistency

Transmission Line Matrix (TLM) network analogues of reversible trapping processes Part B: scaling and consistency Transmission Line Matrix (TLM network analogues of reversible trapping processes Part B: scaling an consistency Donar e Cogan * ANC Eucation, 308-310.A. De Mel Mawatha, Colombo 3, Sri Lanka * onarecogan@gmail.com

More information

Table of Common Derivatives By David Abraham

Table of Common Derivatives By David Abraham Prouct an Quotient Rules: Table of Common Derivatives By Davi Abraham [ f ( g( ] = [ f ( ] g( + f ( [ g( ] f ( = g( [ f ( ] g( g( f ( [ g( ] Trigonometric Functions: sin( = cos( cos( = sin( tan( = sec

More information

Generalization of the persistent random walk to dimensions greater than 1

Generalization of the persistent random walk to dimensions greater than 1 PHYSICAL REVIEW E VOLUME 58, NUMBER 6 DECEMBER 1998 Generalization of the persistent ranom walk to imensions greater than 1 Marián Boguñá, Josep M. Porrà, an Jaume Masoliver Departament e Física Fonamental,

More information

Electric Potential. Slide 1 / 29. Slide 2 / 29. Slide 3 / 29. Slide 4 / 29. Slide 6 / 29. Slide 5 / 29. Work done in a Uniform Electric Field

Electric Potential. Slide 1 / 29. Slide 2 / 29. Slide 3 / 29. Slide 4 / 29. Slide 6 / 29. Slide 5 / 29. Work done in a Uniform Electric Field Slie 1 / 29 Slie 2 / 29 lectric Potential Slie 3 / 29 Work one in a Uniform lectric Fiel Slie 4 / 29 Work one in a Uniform lectric Fiel point a point b The path which the particle follows through the uniform

More information

inflow outflow Part I. Regular tasks for MAE598/494 Task 1

inflow outflow Part I. Regular tasks for MAE598/494 Task 1 MAE 494/598, Fall 2016 Project #1 (Regular tasks = 20 points) Har copy of report is ue at the start of class on the ue ate. The rules on collaboration will be release separately. Please always follow the

More information

Leaving Randomness to Nature: d-dimensional Product Codes through the lens of Generalized-LDPC codes

Leaving Randomness to Nature: d-dimensional Product Codes through the lens of Generalized-LDPC codes Leaving Ranomness to Nature: -Dimensional Prouct Coes through the lens of Generalize-LDPC coes Tavor Baharav, Kannan Ramchanran Dept. of Electrical Engineering an Computer Sciences, U.C. Berkeley {tavorb,

More information

On Characterizing the Delay-Performance of Wireless Scheduling Algorithms

On Characterizing the Delay-Performance of Wireless Scheduling Algorithms On Characterizing the Delay-Performance of Wireless Scheuling Algorithms Xiaojun Lin Center for Wireless Systems an Applications School of Electrical an Computer Engineering, Purue University West Lafayette,

More information

Closed and Open Loop Optimal Control of Buffer and Energy of a Wireless Device

Closed and Open Loop Optimal Control of Buffer and Energy of a Wireless Device Close an Open Loop Optimal Control of Buffer an Energy of a Wireless Device V. S. Borkar School of Technology an Computer Science TIFR, umbai, Inia. borkar@tifr.res.in A. A. Kherani B. J. Prabhu INRIA

More information

The continuity equation

The continuity equation Chapter 6 The continuity equation 61 The equation of continuity It is evient that in a certain region of space the matter entering it must be equal to the matter leaving it Let us consier an infinitesimal

More information

Multi-robot Formation Control Using Reinforcement Learning Method

Multi-robot Formation Control Using Reinforcement Learning Method Multi-robot Formation Control Using Reinforcement Learning Metho Guoyu Zuo, Jiatong Han, an Guansheng Han School of Electronic Information & Control Engineering, Beijing University of Technology, Beijing

More information

LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION

LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION The Annals of Statistics 1997, Vol. 25, No. 6, 2313 2327 LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION By Eva Riccomagno, 1 Rainer Schwabe 2 an Henry P. Wynn 1 University of Warwick, Technische

More information

Perfect Matchings in Õ(n1.5 ) Time in Regular Bipartite Graphs

Perfect Matchings in Õ(n1.5 ) Time in Regular Bipartite Graphs Perfect Matchings in Õ(n1.5 ) Time in Regular Bipartite Graphs Ashish Goel Michael Kapralov Sanjeev Khanna Abstract We consier the well-stuie problem of fining a perfect matching in -regular bipartite

More information

Robustness and Perturbations of Minimal Bases

Robustness and Perturbations of Minimal Bases Robustness an Perturbations of Minimal Bases Paul Van Dooren an Froilán M Dopico December 9, 2016 Abstract Polynomial minimal bases of rational vector subspaces are a classical concept that plays an important

More information

arxiv: v2 [math.st] 29 Oct 2015

arxiv: v2 [math.st] 29 Oct 2015 EXPONENTIAL RANDOM SIMPLICIAL COMPLEXES KONSTANTIN ZUEV, OR EISENBERG, AND DMITRI KRIOUKOV arxiv:1502.05032v2 [math.st] 29 Oct 2015 Abstract. Exponential ranom graph moels have attracte significant research

More information

Introduction to the Vlasov-Poisson system

Introduction to the Vlasov-Poisson system Introuction to the Vlasov-Poisson system Simone Calogero 1 The Vlasov equation Consier a particle with mass m > 0. Let x(t) R 3 enote the position of the particle at time t R an v(t) = ẋ(t) = x(t)/t its

More information

Spring 2016 Network Science

Spring 2016 Network Science Spring 206 Network Science Sample Problems for Quiz I Problem [The Application of An one-imensional Poisson Process] Suppose that the number of typographical errors in a new text is Poisson istribute with

More information

Physics 2212 GJ Quiz #4 Solutions Fall 2015

Physics 2212 GJ Quiz #4 Solutions Fall 2015 Physics 2212 GJ Quiz #4 Solutions Fall 215 I. (17 points) The magnetic fiel at point P ue to a current through the wire is 5. µt into the page. The curve portion of the wire is a semicircle of raius 2.

More information

A new proof of the sharpness of the phase transition for Bernoulli percolation on Z d

A new proof of the sharpness of the phase transition for Bernoulli percolation on Z d A new proof of the sharpness of the phase transition for Bernoulli percolation on Z Hugo Duminil-Copin an Vincent Tassion October 8, 205 Abstract We provie a new proof of the sharpness of the phase transition

More information

Construction of the Electronic Radial Wave Functions and Probability Distributions of Hydrogen-like Systems

Construction of the Electronic Radial Wave Functions and Probability Distributions of Hydrogen-like Systems Construction of the Electronic Raial Wave Functions an Probability Distributions of Hyrogen-like Systems Thomas S. Kuntzleman, Department of Chemistry Spring Arbor University, Spring Arbor MI 498 tkuntzle@arbor.eu

More information

u!i = a T u = 0. Then S satisfies

u!i = a T u = 0. Then S satisfies Deterministic Conitions for Subspace Ientifiability from Incomplete Sampling Daniel L Pimentel-Alarcón, Nigel Boston, Robert D Nowak University of Wisconsin-Maison Abstract Consier an r-imensional subspace

More information

Optimal Control of Spatially Distributed Systems

Optimal Control of Spatially Distributed Systems Optimal Control of Spatially Distribute Systems Naer Motee an Ali Jababaie Abstract In this paper, we stuy the structural properties of optimal control of spatially istribute systems. Such systems consist

More information

2-7. Fitting a Model to Data I. A Model of Direct Variation. Lesson. Mental Math

2-7. Fitting a Model to Data I. A Model of Direct Variation. Lesson. Mental Math Lesson 2-7 Fitting a Moel to Data I BIG IDEA If you etermine from a particular set of ata that y varies irectly or inversely as, you can graph the ata to see what relationship is reasonable. Using that

More information

MA 2232 Lecture 08 - Review of Log and Exponential Functions and Exponential Growth

MA 2232 Lecture 08 - Review of Log and Exponential Functions and Exponential Growth MA 2232 Lecture 08 - Review of Log an Exponential Functions an Exponential Growth Friay, February 2, 2018. Objectives: Review log an exponential functions, their erivative an integration formulas. Exponential

More information

Sensors & Transducers 2015 by IFSA Publishing, S. L.

Sensors & Transducers 2015 by IFSA Publishing, S. L. Sensors & Transucers, Vol. 184, Issue 1, January 15, pp. 53-59 Sensors & Transucers 15 by IFSA Publishing, S. L. http://www.sensorsportal.com Non-invasive an Locally Resolve Measurement of Soun Velocity

More information

DEGREE DISTRIBUTION OF SHORTEST PATH TREES AND BIAS OF NETWORK SAMPLING ALGORITHMS

DEGREE DISTRIBUTION OF SHORTEST PATH TREES AND BIAS OF NETWORK SAMPLING ALGORITHMS DEGREE DISTRIBUTION OF SHORTEST PATH TREES AND BIAS OF NETWORK SAMPLING ALGORITHMS SHANKAR BHAMIDI 1, JESSE GOODMAN 2, REMCO VAN DER HOFSTAD 3, AND JÚLIA KOMJÁTHY3 Abstract. In this article, we explicitly

More information

Physics 2212 K Quiz #2 Solutions Summer 2016

Physics 2212 K Quiz #2 Solutions Summer 2016 Physics 1 K Quiz # Solutions Summer 016 I. (18 points) A positron has the same mass as an electron, but has opposite charge. Consier a positron an an electron at rest, separate by a istance = 1.0 nm. What

More information

Acute sets in Euclidean spaces

Acute sets in Euclidean spaces Acute sets in Eucliean spaces Viktor Harangi April, 011 Abstract A finite set H in R is calle an acute set if any angle etermine by three points of H is acute. We examine the maximal carinality α() of

More information

6 General properties of an autonomous system of two first order ODE

6 General properties of an autonomous system of two first order ODE 6 General properties of an autonomous system of two first orer ODE Here we embark on stuying the autonomous system of two first orer ifferential equations of the form ẋ 1 = f 1 (, x 2 ), ẋ 2 = f 2 (, x

More information

SYNCHRONOUS SEQUENTIAL CIRCUITS

SYNCHRONOUS SEQUENTIAL CIRCUITS CHAPTER SYNCHRONOUS SEUENTIAL CIRCUITS Registers an counters, two very common synchronous sequential circuits, are introuce in this chapter. Register is a igital circuit for storing information. Contents

More information

2.5 SOME APPLICATIONS OF THE CHAIN RULE

2.5 SOME APPLICATIONS OF THE CHAIN RULE 2.5 SOME APPLICATIONS OF THE CHAIN RULE The Chain Rule will help us etermine the erivatives of logarithms an exponential functions a x. We will also use it to answer some applie questions an to fin slopes

More information

On the Connectivity Analysis over Large-Scale Hybrid Wireless Networks

On the Connectivity Analysis over Large-Scale Hybrid Wireless Networks This full text paper was peer reviewe at the irection of IEEE Communications Society subject matter experts for publication in the IEEE INFOCOM proceeings This paper was presente as part of the main Technical

More information

Level Construction of Decision Trees in a Partition-based Framework for Classification

Level Construction of Decision Trees in a Partition-based Framework for Classification Level Construction of Decision Trees in a Partition-base Framework for Classification Y.Y. Yao, Y. Zhao an J.T. Yao Department of Computer Science, University of Regina Regina, Saskatchewan, Canaa S4S

More information

Introduction to Markov Processes

Introduction to Markov Processes Introuction to Markov Processes Connexions moule m44014 Zzis law Gustav) Meglicki, Jr Office of the VP for Information Technology Iniana University RCS: Section-2.tex,v 1.24 2012/12/21 18:03:08 gustav

More information

θ x = f ( x,t) could be written as

θ x = f ( x,t) could be written as 9. Higher orer PDEs as systems of first-orer PDEs. Hyperbolic systems. For PDEs, as for ODEs, we may reuce the orer by efining new epenent variables. For example, in the case of the wave equation, (1)

More information

Tractability results for weighted Banach spaces of smooth functions

Tractability results for weighted Banach spaces of smooth functions Tractability results for weighte Banach spaces of smooth functions Markus Weimar Mathematisches Institut, Universität Jena Ernst-Abbe-Platz 2, 07740 Jena, Germany email: markus.weimar@uni-jena.e March

More information

arxiv: v4 [math.pr] 27 Jul 2016

arxiv: v4 [math.pr] 27 Jul 2016 The Asymptotic Distribution of the Determinant of a Ranom Correlation Matrix arxiv:309768v4 mathpr] 7 Jul 06 AM Hanea a, & GF Nane b a Centre of xcellence for Biosecurity Risk Analysis, University of Melbourne,

More information

THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE

THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE Journal of Soun an Vibration (1996) 191(3), 397 414 THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE E. M. WEINSTEIN Galaxy Scientific Corporation, 2500 English Creek

More information

Survey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013

Survey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013 Survey Sampling Kosuke Imai Department of Politics, Princeton University February 19, 2013 Survey sampling is one of the most commonly use ata collection methos for social scientists. We begin by escribing

More information

On a limit theorem for non-stationary branching processes.

On a limit theorem for non-stationary branching processes. On a limit theorem for non-stationary branching processes. TETSUYA HATTORI an HIROSHI WATANABE 0. Introuction. The purpose of this paper is to give a limit theorem for a certain class of iscrete-time multi-type

More information

A study on ant colony systems with fuzzy pheromone dispersion

A study on ant colony systems with fuzzy pheromone dispersion A stuy on ant colony systems with fuzzy pheromone ispersion Louis Gacogne LIP6 104, Av. Kenney, 75016 Paris, France gacogne@lip6.fr Sanra Sanri IIIA/CSIC Campus UAB, 08193 Bellaterra, Spain sanri@iiia.csic.es

More information

Monotonicity for excited random walk in high dimensions

Monotonicity for excited random walk in high dimensions Monotonicity for excite ranom walk in high imensions Remco van er Hofsta Mark Holmes March, 2009 Abstract We prove that the rift θ, β) for excite ranom walk in imension is monotone in the excitement parameter

More information

Role of parameters in the stochastic dynamics of a stick-slip oscillator

Role of parameters in the stochastic dynamics of a stick-slip oscillator Proceeing Series of the Brazilian Society of Applie an Computational Mathematics, v. 6, n. 1, 218. Trabalho apresentao no XXXVII CNMAC, S.J. os Campos - SP, 217. Proceeing Series of the Brazilian Society

More information

Separation of Variables

Separation of Variables Physics 342 Lecture 1 Separation of Variables Lecture 1 Physics 342 Quantum Mechanics I Monay, January 25th, 2010 There are three basic mathematical tools we nee, an then we can begin working on the physical

More information

Estimation of the Maximum Domination Value in Multi-Dimensional Data Sets

Estimation of the Maximum Domination Value in Multi-Dimensional Data Sets Proceeings of the 4th East-European Conference on Avances in Databases an Information Systems ADBIS) 200 Estimation of the Maximum Domination Value in Multi-Dimensional Data Sets Eleftherios Tiakas, Apostolos.

More information

arxiv: v1 [cond-mat.stat-mech] 9 Jan 2012

arxiv: v1 [cond-mat.stat-mech] 9 Jan 2012 arxiv:1201.1836v1 [con-mat.stat-mech] 9 Jan 2012 Externally riven one-imensional Ising moel Amir Aghamohammai a 1, Cina Aghamohammai b 2, & Mohamma Khorrami a 3 a Department of Physics, Alzahra University,

More information

arxiv: v2 [math.pr] 27 Nov 2018

arxiv: v2 [math.pr] 27 Nov 2018 Range an spee of rotor wals on trees arxiv:15.57v [math.pr] 7 Nov 1 Wilfrie Huss an Ecaterina Sava-Huss November, 1 Abstract We prove a law of large numbers for the range of rotor wals with ranom initial

More information

Prof. Dr. Ibraheem Nasser electric_charhe 9/22/2017 ELECTRIC CHARGE

Prof. Dr. Ibraheem Nasser electric_charhe 9/22/2017 ELECTRIC CHARGE ELECTRIC CHARGE Introuction: Orinary matter consists of atoms. Each atom consists of a nucleus, consisting of protons an neutrons, surroune by a number of electrons. In electricity, the electric charge

More information

CMSC 858F: Algorithmic Game Theory Fall 2010 BGP and Interdomain Routing

CMSC 858F: Algorithmic Game Theory Fall 2010 BGP and Interdomain Routing CMSC 858F: Algorithmic Game Theory Fall 2010 BGP an Interomain Routing Instructor: Mohamma T. Hajiaghayi Scribe: Yuk Hei Chan November 3, 2010 1 Overview In this lecture, we cover BGP (Borer Gateway Protocol)

More information

MATHEMATICS BONUS FILES for faculty and students

MATHEMATICS BONUS FILES for faculty and students MATHMATI BONU FIL for faculty an stuents http://www.onu.eu/~mcaragiu1/bonus_files.html RIVD: May 15, 9 PUBLIHD: May 5, 9 toffel 1 Maxwell s quations through the Major Vector Theorems Joshua toffel Department

More information

A Model of Electron-Positron Pair Formation

A Model of Electron-Positron Pair Formation Volume PROGRESS IN PHYSICS January, 8 A Moel of Electron-Positron Pair Formation Bo Lehnert Alfvén Laboratory, Royal Institute of Technology, S-44 Stockholm, Sween E-mail: Bo.Lehnert@ee.kth.se The elementary

More information

Non-deterministic Social Laws

Non-deterministic Social Laws Non-eterministic Social Laws Michael H. Coen MIT Artificial Intelligence Lab 55 Technology Square Cambrige, MA 09 mhcoen@ai.mit.eu Abstract The paper generalizes the notion of a social law, the founation

More information

CAPACITANCE: CHAPTER 24. ELECTROSTATIC ENERGY and CAPACITANCE. Capacitance and capacitors Storage of electrical energy. + Example: A charged spherical

CAPACITANCE: CHAPTER 24. ELECTROSTATIC ENERGY and CAPACITANCE. Capacitance and capacitors Storage of electrical energy. + Example: A charged spherical CAPACITANCE: CHAPTER 24 ELECTROSTATIC ENERGY an CAPACITANCE Capacitance an capacitors Storage of electrical energy Energy ensity of an electric fiel Combinations of capacitors In parallel In series Dielectrics

More information

Binary Discrimination Methods for High Dimensional Data with a. Geometric Representation

Binary Discrimination Methods for High Dimensional Data with a. Geometric Representation Binary Discrimination Methos for High Dimensional Data with a Geometric Representation Ay Bolivar-Cime, Luis Miguel Corova-Roriguez Universia Juárez Autónoma e Tabasco, División Acaémica e Ciencias Básicas

More information

Laplace s Equation in Cylindrical Coordinates and Bessel s Equation (II)

Laplace s Equation in Cylindrical Coordinates and Bessel s Equation (II) Laplace s Equation in Cylinrical Coorinates an Bessel s Equation (II Qualitative properties of Bessel functions of first an secon kin In the last lecture we foun the expression for the general solution

More information

Nuclear Physics and Astrophysics

Nuclear Physics and Astrophysics Nuclear Physics an Astrophysics PHY-302 Dr. E. Rizvi Lecture 2 - Introuction Notation Nuclies A Nuclie is a particular an is esignate by the following notation: A CN = Atomic Number (no. of Protons) A

More information

A Novel Decoupled Iterative Method for Deep-Submicron MOSFET RF Circuit Simulation

A Novel Decoupled Iterative Method for Deep-Submicron MOSFET RF Circuit Simulation A Novel ecouple Iterative Metho for eep-submicron MOSFET RF Circuit Simulation CHUAN-SHENG WANG an YIMING LI epartment of Mathematics, National Tsing Hua University, National Nano evice Laboratories, an

More information

Abstract A nonlinear partial differential equation of the following form is considered:

Abstract A nonlinear partial differential equation of the following form is considered: M P E J Mathematical Physics Electronic Journal ISSN 86-6655 Volume 2, 26 Paper 5 Receive: May 3, 25, Revise: Sep, 26, Accepte: Oct 6, 26 Eitor: C.E. Wayne A Nonlinear Heat Equation with Temperature-Depenent

More information

arxiv: v1 [cs.it] 21 Aug 2017

arxiv: v1 [cs.it] 21 Aug 2017 Performance Gains of Optimal Antenna Deployment for Massive MIMO ystems Erem Koyuncu Department of Electrical an Computer Engineering, University of Illinois at Chicago arxiv:708.06400v [cs.it] 2 Aug 207

More information

State-Space Model for a Multi-Machine System

State-Space Model for a Multi-Machine System State-Space Moel for a Multi-Machine System These notes parallel section.4 in the text. We are ealing with classically moele machines (IEEE Type.), constant impeance loas, an a network reuce to its internal

More information

A look at Einstein s clocks synchronization

A look at Einstein s clocks synchronization A look at Einstein s clocks synchronization ilton Penha Departamento e Física, Universiae Feeral e Minas Gerais, Brasil. nilton.penha@gmail.com Bernhar Rothenstein Politehnica University of Timisoara,

More information

Short Intro to Coordinate Transformation

Short Intro to Coordinate Transformation Short Intro to Coorinate Transformation 1 A Vector A vector can basically be seen as an arrow in space pointing in a specific irection with a specific length. The following problem arises: How o we represent

More information

Switching Time Optimization in Discretized Hybrid Dynamical Systems

Switching Time Optimization in Discretized Hybrid Dynamical Systems Switching Time Optimization in Discretize Hybri Dynamical Systems Kathrin Flaßkamp, To Murphey, an Sina Ober-Blöbaum Abstract Switching time optimization (STO) arises in systems that have a finite set

More information

ELECTRON DIFFRACTION

ELECTRON DIFFRACTION ELECTRON DIFFRACTION Electrons : wave or quanta? Measurement of wavelength an momentum of electrons. Introuction Electrons isplay both wave an particle properties. What is the relationship between the

More information

Sublinear Time Width-Bounded Separators and Their Application to the Protein Side-Chain Packing Problem

Sublinear Time Width-Bounded Separators and Their Application to the Protein Side-Chain Packing Problem Sublinear Time With-Boune Separators an Their Application to the rotein Sie-Chain acking roblem Bin Fu 1,2 an Zhixiang Chen 3 1 Dept. of Computer Science, University of New Orleans, LA 70148, USA. 2 Research

More information

d-dimensional Arrangement Revisited

d-dimensional Arrangement Revisited -Dimensional Arrangement Revisite Daniel Rotter Jens Vygen Research Institute for Discrete Mathematics University of Bonn Revise version: April 5, 013 Abstract We revisit the -imensional arrangement problem

More information

On the enumeration of partitions with summands in arithmetic progression

On the enumeration of partitions with summands in arithmetic progression AUSTRALASIAN JOURNAL OF COMBINATORICS Volume 8 (003), Pages 149 159 On the enumeration of partitions with summans in arithmetic progression M. A. Nyblom C. Evans Department of Mathematics an Statistics

More information

THE USE OF KIRCHOFF S CURRENT LAW AND CUT-SET EQUATIONS IN THE ANALYSIS OF BRIDGES AND TRUSSES

THE USE OF KIRCHOFF S CURRENT LAW AND CUT-SET EQUATIONS IN THE ANALYSIS OF BRIDGES AND TRUSSES Session TH US O KIRCHO S CURRNT LAW AND CUT-ST QUATIONS IN TH ANALYSIS O BRIDGS AND TRUSSS Ravi P. Ramachanran an V. Ramachanran. Department of lectrical an Computer ngineering, Rowan University, Glassboro,

More information

An M/G/1 Retrial Queue with Priority, Balking and Feedback Customers

An M/G/1 Retrial Queue with Priority, Balking and Feedback Customers Journal of Convergence Information Technology Volume 5 Number April 1 An M/G/1 Retrial Queue with Priority Balking an Feeback Customers Peishu Chen * 1 Yiuan Zhu 1 * 1 Faculty of Science Jiangsu University

More information

Power Generation and Distribution via Distributed Coordination Control

Power Generation and Distribution via Distributed Coordination Control Power Generation an Distribution via Distribute Coorination Control Byeong-Yeon Kim, Kwang-Kyo Oh, an Hyo-Sung Ahn arxiv:407.4870v [math.oc] 8 Jul 204 Abstract This paper presents power coorination, power

More information

A LIMIT THEOREM FOR RANDOM FIELDS WITH A SINGULARITY IN THE SPECTRUM

A LIMIT THEOREM FOR RANDOM FIELDS WITH A SINGULARITY IN THE SPECTRUM Teor Imov r. ta Matem. Statist. Theor. Probability an Math. Statist. Vip. 81, 1 No. 81, 1, Pages 147 158 S 94-911)816- Article electronically publishe on January, 11 UDC 519.1 A LIMIT THEOREM FOR RANDOM

More information

Lower Bounds for Local Monotonicity Reconstruction from Transitive-Closure Spanners

Lower Bounds for Local Monotonicity Reconstruction from Transitive-Closure Spanners Lower Bouns for Local Monotonicity Reconstruction from Transitive-Closure Spanners Arnab Bhattacharyya Elena Grigorescu Mahav Jha Kyomin Jung Sofya Raskhonikova Davi P. Wooruff Abstract Given a irecte

More information

Ramsey numbers of some bipartite graphs versus complete graphs

Ramsey numbers of some bipartite graphs versus complete graphs Ramsey numbers of some bipartite graphs versus complete graphs Tao Jiang, Michael Salerno Miami University, Oxfor, OH 45056, USA Abstract. The Ramsey number r(h, K n ) is the smallest positive integer

More information

Lecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations

Lecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations Lecture XII Abstract We introuce the Laplace equation in spherical coorinates an apply the metho of separation of variables to solve it. This will generate three linear orinary secon orer ifferential equations:

More information