A Laplace type problem for a regular lattice with six obstacles

Size: px
Start display at page:

Download "A Laplace type problem for a regular lattice with six obstacles"

Transcription

1 Reent Advanes in Appied & Biomedia Informatis and Computationa Engineering in Systems Appiations A Lapae type probem for a reguar attie with six obstaes D. Baria, G. Caristi, A. Pugisi University of Messina Department S.E.A. Via dei Verdi, 75, 98- Messina Itay Abstrat: Let be R a, b, ; α) a reguar attie with the fundamenta e as in fig.. In this paper we ompute the probabiity that a random segment of onstant eght ersets a side of the attie. In partiuar when the fundamenta e beomes a retange we obtain the Lapae probabiity. Key Words: Geometri Probabiity, stohasti geometry, random sets, random onvex sets and egra geometry. AMS Cassifiation:6D5, 5A. Setion Let R a, b, ) be the reguar attie with fundamenta e is as in fig. : a O A A x B' y 9 A B'' A b B B 6 O 7 C 8 5 O 5 a b fig. b that a segment s erset a side of the fundamenta e C ) we have The obstaes are squares with the side of ength. Considering a random segment whose ength < min a, b) we to want ompute the probabiity that a segment ersets a side of the attie. This probabiity is equa to the probabiity P ) area C ) = ab 8 8 = ab. ) Considering now a position s of the segment with baryenter p and whih forms an ange with axis x. We onsider the imit positions of the segment s for a determinated ange, and et Ĉ) ) the figure determinated by these positions see fig. ): h F E E' F D' 6 D D'' 5 F 9 E F' O F E O fig. Let a, a,..., a 9 the poygons of the fig. suh that: areaĉ) ) = areac ) area a ) + area a ) + area a ) +area a ) + area a 5 ) + area a 6 ) + area a 7 ) +area a 8 ) + area a 9 ). ) Considering AB = x, A B = y, from triange AA B foow that x = tg, ) area a ) = x = tg. ) 8 From triange A A A we have that A A = tg, 5) O 6 ISBN:

2 Reent Advanes in Appied & Biomedia Informatis and Computationa Engineering in Systems Appiations E ' area a ) = A A = tg. 6) 8 F / Considering the 5), the paraeogram A B F F A F = a A A = a tg, / F h fig. E E / E h = os, area a ) = A F h = a ) os sin. 7) foow that E E = tg, F E = b E E = b tg, h = sin, area a 5 ) = F E h = b tg ) sin = In order to ompute the area of the poygon a onsidering the figure F b ) sin os. 9) In the same way we have that F ' / h C area a 8 ) = E E = tg. ) 8 F F From triange E D D we have that D D = tg, ) fig. We have F F F = =, h = sin + ) = sin + ) = area a 7 ) = D D = tg. ) and os + sin ), area a ) = h 8 = os + sin ) 8. 8) Compute now the area of the paraeogram a 5. From fig. From figure 5 D D D' h fig.5 D' ' ISBN:

3 Reent Advanes in Appied & Biomedia Informatis and Computationa Engineering in Systems Appiations we have D D = D D +, DD = E D =, and onsidering the ), we have that D D = tg +, and sine D DD =, From here B B = b x = b os, area a 9 ) = b ) os sin. 5) Considering the formue ), 6), 7), 8), 9), ), ), ) and ) in the ) we obtain that: h = D D sin ) = Then sin + os. area a 6 ) = tg + ) os = DD h = 8 sin + os ) 8. ) From fig. 6 A A x B ' ' foow that B ' a9 h fig.6 h = sin, B B / area a 9 ) = B B h = B B sin. From triange O B A we have that x + = os, ) x = os. areaĉ) ) = areac ) tg + tg + a ) os sin + os + sin ) tg+ b ) sin os + sin + os ) + tg + tg+ b ) os sin. 6) Considering A A = z, from the trianges AA B and A A A we obtain that y y = = sin, z = os, sin, z = os and sine y + z =, we have sin + os =. Mutipe the i two members of this reation before with sin and after with os, we obtain tg = sin, tg = os. Considering this reation in 5) we have that area Ĉ) ) = areac ) ISBN:

4 Reent Advanes in Appied & Biomedia Informatis and Computationa Engineering in Systems Appiations a + ) os + b ) sin sin. 7) Denoting with M the set of segments s whose baryenter are in C ) and N the set of segments s whose baryenter are in C ) that do not erset the boundary of C ), we have P ) = µ N ) µ M ), 8) where µ is the Lebesgue measure in Euidean pane. In order to ompute the measures µ M ) and µ N ) we use the Poinaré kinemati measure dk = dx dy, where x, y are the oordinates of p and the defined ange. Considering that,, we have that µ M ) = and by 6) µ N ) = x,y) C ) area C) 9) x,y) Ĉ) ) area Ĉ) ) = areac) a + ) + b ). ) Considering the 7), 8) and 9) we obtain the probabiity: = a + b ) ab = ) P ) a + b ) ab ) When the fundamenta e C ) beomes a retange with sides a and b and the obstaes beome pos and the probabiity P ) beomes the Lapae probabiity: Setion P = a + b + ). a b + ) Let be R a, b, ) the reguar attie with fundamenta e is as in fig. 7. Fig ) C fig.7 Denoting with C ) the fundamenta e, we have: area C ) = ab. ) The e C ) have six obstaes that are squares with diagona of eght with < min a, b). Considering a segment s of random position and of eght with < < min a, b), we want ompute the probabitiy that this segment ersets a side of attie. This probabiity is equa to probabiity P ) that the segment s ersets the bounderay of the fundamenta e. The position of the segment s is determinated by the midde po p and by the ange that the segment form with the axis x. We onsider the imit positions of the segment s that orrisponde at ange and et Ĉ) ) the determinated figure from this position see fig. 8): a b / / a a a a Fig ) C ) fig.8 b ISBN:

5 Reent Advanes in Appied & Biomedia Informatis and Computationa Engineering in Systems Appiations From this figure we an write: areaĉ) ) = areac ) areab ) + areab ) + areab ) + areab ). ) Considering some resuts that we have obtained in a previous paper, foow that: areaĉ) ) = ab a ) os + b ) sin + sin + ) os sin = ab a + ) os + b ) sin sin. ) Denoting with M the set of segments s whose the midde po are in C ) and N the set of segments s whose the midde po are in C ), we have that: P ) = µ N ) µ M ), ) where µ is the Lebesgue measure in Euidean pane. In order to ompute the measures µ M ) and µ N ) we use the Poinaré kinemati measure dk = dx dy, area C ) ) = ab ) a + ) os + b ) sin sin = ab ) a + b ). 6) Considering the ), ) and 5) we obtain the probabiity: P ) a + b) = ab. 7) ) When, the obstaes beames pos and the fundamenta e beames a retange with side a and b. In this ase the probabiity 7) beomes the Lapae probabiity: Setion P = a + b). ab Let R a, b, ; α) be the reguar attie with fundamenta e C ) is as in fig.. a α b ) C ) b where x, y are the oordinates of p and the defined ange. Sine,, we obtain that: Fig 7 fig.9 µ M ) = x,y) C ) areac) = ab ). 5) and onsidering the ) µ N ) = x,y) Ĉ) ) where α, is an ange and < min a, b). The C ) have six obstaes that are rhombs with side and with the diagonas d = sin α, d = os α. We have that: areac ) = ab + a os α + b sin α) + sin α os α. In the same way of the Setion, denoting with Ĉ ) ) the figure determinated by the imit positions of the segments s for a assigned vaue of see fig. ): ISBN:

6 Reent Advanes in Appied & Biomedia Informatis and Computationa Engineering in Systems Appiations m m m m m5 ) C ) sin tgα os tgα) = areac) a + b + os α + sin α) 5 fig. Fig 8 From this figure we an write: sin α) + areaĉ) ) = areac ) a sin α) os α os + b sin + sin + α) + sin α) = areac ) a + sin α + os α) os + b+ os α + sin α) sin sin tgα os tgα) 8) Denoting with M the set of segments s whose the midde po are in C ) and N the set of segments s whose the midde po are in C ), we have that: P ) = µ N ) µ M ). 9) Sine,, we obtain that: tgα). ) Considering the 9) and ) in 8) we obtain that: P ) = a + b + os α + sin α) ab + a os α + b sin α) + sin α os α. ) When, the obstaes beames segments of enght that go in the ounderay of the attie, the fundamenta e C ) beames a retange of side a and b + and the ) beomes the Lapae probabiity: Referenes: P = a + b + ). a b + ) Caristi G and Stoka M., A Lapae type probem for a reguar attie with obstaes I), Atti A. Si. Torino, to appear). Caristi G and Stoka M., A Lapae type probem for a reguar attie with obstaes II), Atti A. Si. Torino, to appear). Poinaré H., Cau des probabiitiés, ed., Carré, Paris, 9. Stoka M., Probabiités géométriques de type Buffon dans e pan euidean, Atti A. Si. Torino, T., pp. 5-59, µ M ) = x,y) C ) and areac), ) µ N ) = areac) x,y) Ĉ) ) a + sin α + os α) os + b + os α + sin α) sin ISBN:

A Buffon - Laplace Type Problems for an Irregular Lattice and with Maximum Probability

A Buffon - Laplace Type Problems for an Irregular Lattice and with Maximum Probability Applied Mathematical Sciences, Vol. 8,, no. 65, 887-893 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/.988/ams..96 A Buffon - Laplace Type Problems for an Irregular Lattice and with Maximum Probability

More information

A Laplace Type Problems for a Lattice with Cell Composed by Three Quadrilaterals and with Maximum Probability

A Laplace Type Problems for a Lattice with Cell Composed by Three Quadrilaterals and with Maximum Probability Applied Mathematical Sciences, Vol. 8, 1, no. 165, 879-886 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/1.1988/ams.1.11915 A Laplace Type Problems for a Lattice with Cell Composed by Three Quadrilaterals

More information

Laplace Type Problem with Non-uniform Distribution

Laplace Type Problem with Non-uniform Distribution Applied Mathematical Sciences, Vol. 1, 16, no. 3, 1595-16 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/1.1988/ams.16.66 Laplace Type Problem with Non-uniform Distribution Giuseppe Caristi Department

More information

Buffon-Laplace Type Problem for an Irregular Lattice

Buffon-Laplace Type Problem for an Irregular Lattice Applied Mathematical Sciences Vol. 11 17 no. 15 731-737 HIKARI Ltd www.m-hikari.com https://doi.org/1.1988/ams.17.783 Buffon-Laplace Type Problem for an Irregular Lattice Ersilia Saitta Department of Economics

More information

Extensions of Laplace Type Problems in the Euclidean Space

Extensions of Laplace Type Problems in the Euclidean Space Internationa Mathematica Forum, Vo. 9, 214, no. 26, 1253-1259 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/1.12988/imf.214.46112 Extensions of Lapace Type Probems in the Eucidean Space Giuseppe Caristi

More information

A Laplace Type Problem for a Regular Lattice with Convex-Concave Cell with Obstacles Rhombus

A Laplace Type Problem for a Regular Lattice with Convex-Concave Cell with Obstacles Rhombus International Journal of Conteporary Matheatical Sciences Vol. 9, 14, no. 1, 479-45 HIKARI Ltd, www.-hikari.co http://dx.doi.org/1.19/ijcs.14.4659 A Laplace Type Proble for a Regular Lattice with Convex-Concave

More information

The Square of the Dirichlet-to-Neumann map equals minus Laplacian

The Square of the Dirichlet-to-Neumann map equals minus Laplacian The Square of the Dirihet-to-Neumann map equas minus Lapaian D V Ingerman Abstrat. The Dirihet-to-Neumann maps onnet boundary vaues of harmoni funtions. It is an amazing fat that the square of the non-oa

More information

Riassunto. Si risolvono problemi di tipo Buffon per un corpo test arbitrario e una speciale configurazione di linee nel piano Euclideo.

Riassunto. Si risolvono problemi di tipo Buffon per un corpo test arbitrario e una speciale configurazione di linee nel piano Euclideo. Acc. Sc. Torino Atti Sc. Fis. 4 (26), 83-9. GEOMETRIA Riassunto. Si risolvono problemi di tipo Buffon per un corpo test arbitrario e una speciale configurazione di linee nel piano Euclideo. Abstract. We

More information

Applied Mathematical Sciences, Vol. 10, 2016, no. 34, HIKARI Ltd,

Applied Mathematical Sciences, Vol. 10, 2016, no. 34, HIKARI Ltd, Applied Mathematical Sciences, Vol. 10, 016, no. 34, 1663-1681 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.1988/ams.016.63109 Analysis of the Railway Network Operations Safety, with of Different

More information

The Binary Space Partitioning-Tree Process Supplementary Material

The Binary Space Partitioning-Tree Process Supplementary Material The inary Space Partitioning-Tree Process Suppementary Materia Xuhui Fan in Li Scott. Sisson Schoo of omputer Science Fudan University ibin@fudan.edu.cn Schoo of Mathematics and Statistics University of

More information

PROCEEDINGS OF THE YEREVAN STATE UNIVERSITY GEOMETRIC PROBABILITY CALCULATION FOR A TRIANGLE

PROCEEDINGS OF THE YEREVAN STATE UNIVERSITY GEOMETRIC PROBABILITY CALCULATION FOR A TRIANGLE PROCEEDINGS OF THE YEREVAN STATE UNIVERSITY Physica and Mathematica Sciences 07, 5(3, p. 6 M a t h e m a t i c s GEOMETRIC PROBABILITY CALCULATION FOR A TRIANGLE N. G. AHARONYAN, H. O. HARUTYUNYAN Chair

More information

Research Article Some Applications of Second-Order Differential Subordination on a Class of Analytic Functions Defined by Komatu Integral Operator

Research Article Some Applications of Second-Order Differential Subordination on a Class of Analytic Functions Defined by Komatu Integral Operator ISRN Mathematia Anaysis, Artie ID 66235, 5 pages http://dx.doi.org/1.1155/214/66235 Researh Artie Some Appiations of Seond-Order Differentia Subordination on a Cass of Anayti Funtions Defined by Komatu

More information

THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE

THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE KATIE L. MAY AND MELISSA A. MITCHELL Abstract. We show how to identify the minima path network connecting three fixed points on

More information

Discovery of Non-Euclidean Geometry

Discovery of Non-Euclidean Geometry iscovery of Non-Eucidean Geometry pri 24, 2013 1 Hyperboic geometry János oyai (1802-1860), ar Friedrich Gauss (1777-1855), and Nikoai Ivanovich Lobachevsky (1792-1856) are three founders of non-eucidean

More information

2M2. Fourier Series Prof Bill Lionheart

2M2. Fourier Series Prof Bill Lionheart M. Fourier Series Prof Bi Lionheart 1. The Fourier series of the periodic function f(x) with period has the form f(x) = a 0 + ( a n cos πnx + b n sin πnx ). Here the rea numbers a n, b n are caed the Fourier

More information

LECTURE 2 Geometrical Properties of Rod Cross Sections (Part 2) 1 Moments of Inertia Transformation with Parallel Transfer of Axes.

LECTURE 2 Geometrical Properties of Rod Cross Sections (Part 2) 1 Moments of Inertia Transformation with Parallel Transfer of Axes. V. DEMENKO MECHNCS OF MTERLS 05 LECTURE Geometrial Properties of Rod Cross Setions (Part ) Moments of nertia Transformation with Parallel Transfer of xes. Parallel-xes Theorems S Given: a b = S = 0. z

More information

EXACT TRAVELLING WAVE SOLUTIONS FOR THE GENERALIZED KURAMOTO-SIVASHINSKY EQUATION

EXACT TRAVELLING WAVE SOLUTIONS FOR THE GENERALIZED KURAMOTO-SIVASHINSKY EQUATION Journal of Mathematial Sienes: Advanes and Appliations Volume 3, 05, Pages -3 EXACT TRAVELLING WAVE SOLUTIONS FOR THE GENERALIZED KURAMOTO-SIVASHINSKY EQUATION JIAN YANG, XIAOJUAN LU and SHENGQIANG TANG

More information

ABSOLUTELY CONTINUOUS FUNCTIONS OF TWO VARIABLES IN THE SENSE OF CARATHÉODORY

ABSOLUTELY CONTINUOUS FUNCTIONS OF TWO VARIABLES IN THE SENSE OF CARATHÉODORY Eetroni Journa of Differentia Equations, Vo. 2010(2010), No. 154, pp. 1 11. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu ABSOLUTELY CONTINUOUS

More information

FOR many years the authors of this paper have worked on

FOR many years the authors of this paper have worked on The Fast Parametri Integra Equations System for Poygona D Potentia Probems Andrzej Kużeewski and Eugeniusz Zieniuk Abstrat Appiation of tehniques for modeing of boundary vaue probems impies three onfiting

More information

max min z i i=1 x j k s.t. j=1 x j j:i T j

max min z i i=1 x j k s.t. j=1 x j j:i T j AM 221: Advaned Optimization Spring 2016 Prof. Yaron Singer Leture 22 April 18th 1 Overview In this leture, we will study the pipage rounding tehnique whih is a deterministi rounding proedure that an be

More information

). In accordance with the Lorentz transformations for the space-time coordinates of the same event, the space coordinates become

). In accordance with the Lorentz transformations for the space-time coordinates of the same event, the space coordinates become Relativity and quantum mehanis: Jorgensen 1 revisited 1. Introdution Bernhard Rothenstein, Politehnia University of Timisoara, Physis Department, Timisoara, Romania. brothenstein@gmail.om Abstrat. We first

More information

Using the Green s Function to find the Solution to the Wave. Equation:

Using the Green s Function to find the Solution to the Wave. Equation: Using the Green s Funtion to find the Soution to the Wave Exampe 1: 2 1 2 2 t 2 Equation: r,t q 0 e it r aẑ r aẑ r,t r 1 r ; r r,t r 1 r 2 The Green s funtion soution is given by r,t G R r r,t t Fr,t d

More information

Assignment 7 Due Tuessday, March 29, 2016

Assignment 7 Due Tuessday, March 29, 2016 Math 45 / AMCS 55 Dr. DeTurck Assignment 7 Due Tuessday, March 9, 6 Topics for this week Convergence of Fourier series; Lapace s equation and harmonic functions: basic properties, compuations on rectanges

More information

distibution. G. Caristi - E. Saitta and M. Stoka

distibution. G. Caristi - E. Saitta and M. Stoka A Laplace type problem with non uniform distribution G. Caristi - E. Saitta and M. Stoka Abstract - In some previous papers the authors consider some Laplace type problem for different lattice, in particular

More information

Lecture 17 - The Secrets we have Swept Under the Rug

Lecture 17 - The Secrets we have Swept Under the Rug Lecture 17 - The Secrets we have Swept Under the Rug Today s ectures examines some of the uirky features of eectrostatics that we have negected up unti this point A Puzze... Let s go back to the basics

More information

SEMINAR 2. PENDULUMS. V = mgl cos θ. (2) L = T V = 1 2 ml2 θ2 + mgl cos θ, (3) d dt ml2 θ2 + mgl sin θ = 0, (4) θ + g l

SEMINAR 2. PENDULUMS. V = mgl cos θ. (2) L = T V = 1 2 ml2 θ2 + mgl cos θ, (3) d dt ml2 θ2 + mgl sin θ = 0, (4) θ + g l Probem 7. Simpe Penduum SEMINAR. PENDULUMS A simpe penduum means a mass m suspended by a string weightess rigid rod of ength so that it can swing in a pane. The y-axis is directed down, x-axis is directed

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION DOI: 10.1038/NPHOTON.013.10 Suppementary Information: Quantum teeportation using a ight emitting diode J. Nisson 1, R. M. Stevenson 1*, K. H. A. Chan 1,, J. Skiba-Szymanska 1, M. Luamarini 1, M. B. Ward

More information

Bourgain s Theorem. Computational and Metric Geometry. Instructor: Yury Makarychev. d(s 1, s 2 ).

Bourgain s Theorem. Computational and Metric Geometry. Instructor: Yury Makarychev. d(s 1, s 2 ). Bourgain s Theorem Computationa and Metric Geometry Instructor: Yury Makarychev 1 Notation Given a metric space (X, d) and S X, the distance from x X to S equas d(x, S) = inf d(x, s). s S The distance

More information

LONGITUDINAL NATURAL FREQUENCIES OF RODS AND RESPONSE TO INITIAL CONDITIONS Revision B

LONGITUDINAL NATURAL FREQUENCIES OF RODS AND RESPONSE TO INITIAL CONDITIONS Revision B By Tom Irvine Email: tomirvine@aol.om ONGITUDINA NATURA FREQUENCIES OF RODS AND RESPONSE TO INITIA CONDITIONS Revision B Marh 4, 009 Consider a thin rod. E, A, m E is the modulus of elastiity. A is the

More information

CONTINUATION OF SAKSHI VIDYA PAGE ( ) PAIR OF STRAIGHT LINES

CONTINUATION OF SAKSHI VIDYA PAGE ( ) PAIR OF STRAIGHT LINES CONTINUATION OF SAKSHI VIDYA PAGE (0--008) A Bhanu Kumar, Senior Faulty, Sri Chaitanya Eduational Institutions, Hyderaad PAIR OF STRAIGHT LINES (I Year Inter) * If S = af ax + hxy + y + gx + fy + represent

More information

The casing is subjected to the following:

The casing is subjected to the following: 16.50 Leture 13 Subjet: Roket asing design; Strutural modeling Thus far all our modeling has dealt with the fluid mehanis and thermodynamis of rokets. This is appropriate beause it is these features that

More information

Advanced Computational Fluid Dynamics AA215A Lecture 4

Advanced Computational Fluid Dynamics AA215A Lecture 4 Advaned Computational Fluid Dynamis AA5A Leture 4 Antony Jameson Winter Quarter,, Stanford, CA Abstrat Leture 4 overs analysis of the equations of gas dynamis Contents Analysis of the equations of gas

More information

arxiv:gr-qc/ v2 6 Feb 2004

arxiv:gr-qc/ v2 6 Feb 2004 Hubble Red Shift and the Anomalous Aeleration of Pioneer 0 and arxiv:gr-q/0402024v2 6 Feb 2004 Kostadin Trenčevski Faulty of Natural Sienes and Mathematis, P.O.Box 62, 000 Skopje, Maedonia Abstrat It this

More information

Joel Broida UCSD Fall 2009 Phys 130B QM II. Homework Set 2 DO ALL WORK BY HAND IN OTHER WORDS, DON T USE MATHEMAT- ICA OR ANY CALCULATORS.

Joel Broida UCSD Fall 2009 Phys 130B QM II. Homework Set 2 DO ALL WORK BY HAND IN OTHER WORDS, DON T USE MATHEMAT- ICA OR ANY CALCULATORS. Joe Broida UCSD Fa 009 Phys 30B QM II Homework Set DO ALL WORK BY HAND IN OTHER WORDS, DON T USE MATHEMAT- ICA OR ANY CALCULATORS. You may need to use one or more of these: Y 0 0 = 4π Y 0 = 3 4π cos Y

More information

Lecture Notes for Math 251: ODE and PDE. Lecture 34: 10.7 Wave Equation and Vibrations of an Elastic String

Lecture Notes for Math 251: ODE and PDE. Lecture 34: 10.7 Wave Equation and Vibrations of an Elastic String ecture Notes for Math 251: ODE and PDE. ecture 3: 1.7 Wave Equation and Vibrations of an Eastic String Shawn D. Ryan Spring 212 ast Time: We studied other Heat Equation probems with various other boundary

More information

Available online at ScienceDirect

Available online at   ScienceDirect Avaiabe onine at www.sienediret.om SieneDiret Proedia Engineering 7 04 ) 9 4 Geoogia Engineering Driing Tehnoog Conferene IGEDTC), New Internationa Convention Eposition Center Chengdu Centur Cit on rd-5th

More information

the following action R of T on T n+1 : for each θ T, R θ : T n+1 T n+1 is defined by stated, we assume that all the curves in this paper are defined

the following action R of T on T n+1 : for each θ T, R θ : T n+1 T n+1 is defined by stated, we assume that all the curves in this paper are defined How should a snake turn on ie: A ase study of the asymptoti isoholonomi problem Jianghai Hu, Slobodan N. Simić, and Shankar Sastry Department of Eletrial Engineering and Computer Sienes University of California

More information

A model for measurement of the states in a coupled-dot qubit

A model for measurement of the states in a coupled-dot qubit A model for measurement of the states in a oupled-dot qubit H B Sun and H M Wiseman Centre for Quantum Computer Tehnology Centre for Quantum Dynamis Griffith University Brisbane 4 QLD Australia E-mail:

More information

22.54 Neutron Interactions and Applications (Spring 2004) Chapter 6 (2/24/04) Energy Transfer Kernel F(E E')

22.54 Neutron Interactions and Applications (Spring 2004) Chapter 6 (2/24/04) Energy Transfer Kernel F(E E') 22.54 Neutron Interations and Appliations (Spring 2004) Chapter 6 (2/24/04) Energy Transfer Kernel F(E E') Referenes -- J. R. Lamarsh, Introdution to Nulear Reator Theory (Addison-Wesley, Reading, 1966),

More information

Investigation of the de Broglie-Einstein velocity equation s. universality in the context of the Davisson-Germer experiment. Yusuf Z.

Investigation of the de Broglie-Einstein velocity equation s. universality in the context of the Davisson-Germer experiment. Yusuf Z. Investigation of the de Broglie-instein veloity equation s universality in the ontext of the Davisson-Germer experiment Yusuf Z. UMUL Canaya University, letroni and Communiation Dept., Öğretmenler Cad.,

More information

A Laplace Type Problem for a Lattice with Non-convex Cells and with a Rectangle Body Test

A Laplace Type Problem for a Lattice with Non-convex Cells and with a Rectangle Body Test Interntionl Journl of Mthemticl Anlysis Vol. 9, 15, no. 38, 1895-19 HIKARI Ltd, www.m-hikri.com http://dx.doi.org/1.1988/ijm.15.519 A Lplce Type Problem for Lttice with Non-convex Cells nd with Rectngle

More information

On some problems of synthesis of spatial five-bar hinged mechanisms with two degrees of freedom

On some problems of synthesis of spatial five-bar hinged mechanisms with two degrees of freedom Internationa Journa of Mechanica Engineering and Appications 014 (6): 104-110 Puished onine ecemer 18, 014 (http://www.sciencepuishinggroup.com/j/ijmea) doi: 10.11648/j.ijmea.014006.14 ISSN: 330-03X (Print)

More information

MA2331 Tutorial Sheet 5, Solutions December 2014 (Due 12 December 2014 in class) F = xyi+ 1 2 x2 j+k = φ (1)

MA2331 Tutorial Sheet 5, Solutions December 2014 (Due 12 December 2014 in class) F = xyi+ 1 2 x2 j+k = φ (1) MA2331 Tutorial Sheet 5, Solutions. 1 4 Deember 214 (Due 12 Deember 214 in lass) Questions 1. ompute the line integrals: (a) (dx xy + 1 2 dy x2 + dz) where is the line segment joining the origin and the

More information

The Hanging Chain. John McCuan. January 19, 2006

The Hanging Chain. John McCuan. January 19, 2006 The Hanging Chain John MCuan January 19, 2006 1 Introdution We onsider a hain of length L attahed to two points (a, u a and (b, u b in the plane. It is assumed that the hain hangs in the plane under a

More information

656 F. C. Aaraz and R. Z. Bariev terhange positions, that is, there is no reations. In this paper we extend the asymmetri diffusion probem with N type

656 F. C. Aaraz and R. Z. Bariev terhange positions, that is, there is no reations. In this paper we extend the asymmetri diffusion probem with N type Braziian Journa of Physis, vo. 30, no. 4, Deember, 2000 655 Exat Soution of Asymmetri Diffusion With N Casses of Parties of Arbitrary Size and Hierarhia Order F. C. Aaraz Departamento de F sia, Universidade

More information

arxiv:cond-mat/ v1 [cond-mat.dis-nn] 13 Feb 2003

arxiv:cond-mat/ v1 [cond-mat.dis-nn] 13 Feb 2003 arxiv:cond-mat/369v [cond-mat.dis-nn] 3 Feb 3 Brownian Motion in wedges, ast passage time and the second arc-sine aw Aain Comtet, and Jean Desbois nd February 8 Laboratoire de Physique Théorique et Modèes

More information

Add Math (4044/02) (+) x (+) 2. Find the coordinates of the points of intersection of the curve xy 2 the line 2y 1 x 0. [5]

Add Math (4044/02) (+) x (+) 2. Find the coordinates of the points of intersection of the curve xy 2 the line 2y 1 x 0. [5] Add Math (444/) Requirement : Answer a questions Tota mars : 7 Duration : hour 45 minutes. Sove the inequaity 5 and represent the soution set on the number ine. [4] 5 4 From the setch on number ine, we

More information

Lecture 9. Stability of Elastic Structures. Lecture 10. Advanced Topic in Column Buckling

Lecture 9. Stability of Elastic Structures. Lecture 10. Advanced Topic in Column Buckling Lecture 9 Stabiity of Eastic Structures Lecture 1 Advanced Topic in Coumn Bucking robem 9-1: A camped-free coumn is oaded at its tip by a oad. The issue here is to find the itica bucking oad. a) Suggest

More information

The Group Structure on a Smooth Tropical Cubic

The Group Structure on a Smooth Tropical Cubic The Group Structure on a Smooth Tropica Cubic Ethan Lake Apri 20, 2015 Abstract Just as in in cassica agebraic geometry, it is possibe to define a group aw on a smooth tropica cubic curve. In this note,

More information

2.1. Cantilever The Hooke's law

2.1. Cantilever The Hooke's law .1. Cantiever.1.1 The Hooke's aw The cantiever is the most common sensor of the force interaction in atomic force microscopy. The atomic force microscope acquires any information about a surface because

More information

Research Article Approximation of Analytic Functions by Solutions of Cauchy-Euler Equation

Research Article Approximation of Analytic Functions by Solutions of Cauchy-Euler Equation Funtion Spaes Volume 2016, Artile ID 7874061, 5 pages http://d.doi.org/10.1155/2016/7874061 Researh Artile Approimation of Analyti Funtions by Solutions of Cauhy-Euler Equation Soon-Mo Jung Mathematis

More information

Electromagnetic radiation of the travelling spin wave propagating in an antiferromagnetic plate. Exact solution.

Electromagnetic radiation of the travelling spin wave propagating in an antiferromagnetic plate. Exact solution. arxiv:physis/99536v1 [physis.lass-ph] 15 May 1999 Eletromagneti radiation of the travelling spin wave propagating in an antiferromagneti plate. Exat solution. A.A.Zhmudsky November 19, 16 Abstrat The exat

More information

XSAT of linear CNF formulas

XSAT of linear CNF formulas XSAT of inear CN formuas Bernd R. Schuh Dr. Bernd Schuh, D-50968 Kön, Germany; bernd.schuh@netcoogne.de eywords: compexity, XSAT, exact inear formua, -reguarity, -uniformity, NPcompeteness Abstract. Open

More information

Course 2BA1, Section 11: Periodic Functions and Fourier Series

Course 2BA1, Section 11: Periodic Functions and Fourier Series Course BA, 8 9 Section : Periodic Functions and Fourier Series David R. Wikins Copyright c David R. Wikins 9 Contents Periodic Functions and Fourier Series 74. Fourier Series of Even and Odd Functions...........

More information

Tracking Control of Multiple Mobile Robots

Tracking Control of Multiple Mobile Robots Proceedings of the 2001 IEEE Internationa Conference on Robotics & Automation Seou, Korea May 21-26, 2001 Tracking Contro of Mutipe Mobie Robots A Case Study of Inter-Robot Coision-Free Probem Jurachart

More information

Module 22: Simple Harmonic Oscillation and Torque

Module 22: Simple Harmonic Oscillation and Torque Modue : Simpe Harmonic Osciation and Torque.1 Introduction We have aready used Newton s Second Law or Conservation of Energy to anayze systems ike the boc-spring system that osciate. We sha now use torque

More information

Chapter-3 PERFORMANCE MEASURES OF A MULTI-EVAPORATOR TYPE COMPRESSOR WITH STANDBY EXPANSION VALVE

Chapter-3 PERFORMANCE MEASURES OF A MULTI-EVAPORATOR TYPE COMPRESSOR WITH STANDBY EXPANSION VALVE Chapter-3 PERFRMANCE MEASURES F A MUTI-EVAPRATR TYPE CMPRESSR WITH STANDBY EXPANSIN VAVE 3. INTRDUCTIN In this model, the author has onsidered a refrigeration plant whih ontains a single ompressor with

More information

ON A PROCESS DERIVED FROM A FILTERED POISSON PROCESS

ON A PROCESS DERIVED FROM A FILTERED POISSON PROCESS ON A PROCESS DERIVED FROM A FILTERED POISSON PROCESS MARIO LEFEBVRE and JEAN-LUC GUILBAULT A ontinuous-time and ontinuous-state stohasti proess, denoted by {Xt), t }, is defined from a proess known as

More information

THE NUMERICAL EVALUATION OF THE LEVITATION FORCE IN A HYDROSTATIC BEARING WITH ALTERNATING POLES

THE NUMERICAL EVALUATION OF THE LEVITATION FORCE IN A HYDROSTATIC BEARING WITH ALTERNATING POLES THE NUMERICAL EVALUATION OF THE LEVITATION FORCE IN A HYDROSTATIC BEARING WITH ALTERNATING POLES MARIAN GRECONICI Key words: Magnetic iquid, Magnetic fied, 3D-FEM, Levitation, Force, Bearing. The magnetic

More information

Strauss PDEs 2e: Section Exercise 1 Page 1 of 7

Strauss PDEs 2e: Section Exercise 1 Page 1 of 7 Strauss PDEs 2e: Section 4.3 - Exercise 1 Page 1 of 7 Exercise 1 Find the eigenvaues graphicay for the boundary conditions X(0) = 0, X () + ax() = 0. Assume that a 0. Soution The aim here is to determine

More information

Chapter 2: Solution of First order ODE

Chapter 2: Solution of First order ODE 0 Chapter : Solution of irst order ODE Se. Separable Equations The differential equation of the form that is is alled separable if f = h g; In order to solve it perform the following steps: Rewrite the

More information

67. Which reason and statement are missing from the following proof? B C. Given

67. Which reason and statement are missing from the following proof? B C. Given Acceerated Math : Wednesday, January 11, 2006, 9:49:53 AM Page 1 Dr. Kevin Kiyoi Geometry 10, Per 4 Amador Vaey Form Number 96140 Practice Geo Objectives: (5 of 5 isted) 31. Proofs: Agebra & properties

More information

Time-varying Stiffness Characteristics of Shaft with Slant Crack

Time-varying Stiffness Characteristics of Shaft with Slant Crack Internationa Conferene on Modeing, Simuation and Appied Mathematis (MSAM 05) Time-varying Stiffness Charateristis of Shaft with Sant Cra Hengheng Xia Shoo of Aeronautia Manufaturing Engineering Nanhang

More information

FOURIER SERIES ON ANY INTERVAL

FOURIER SERIES ON ANY INTERVAL FOURIER SERIES ON ANY INTERVAL Overview We have spent considerabe time earning how to compute Fourier series for functions that have a period of 2p on the interva (-p,p). We have aso seen how Fourier series

More information

2. The Energy Principle in Open Channel Flows

2. The Energy Principle in Open Channel Flows . The Energy Priniple in Open Channel Flows. Basi Energy Equation In the one-dimensional analysis of steady open-hannel flow, the energy equation in the form of Bernoulli equation is used. Aording to this

More information

Relativity fundamentals explained well (I hope) Walter F. Smith, Haverford College

Relativity fundamentals explained well (I hope) Walter F. Smith, Haverford College Relativity fundamentals explained well (I hope) Walter F. Smith, Haverford College 3-14-06 1 Propagation of waves through a medium As you ll reall from last semester, when the speed of sound is measured

More information

Taste for variety and optimum product diversity in an open economy

Taste for variety and optimum product diversity in an open economy Taste for variety and optimum produt diversity in an open eonomy Javier Coto-Martínez City University Paul Levine University of Surrey Otober 0, 005 María D.C. Garía-Alonso University of Kent Abstrat We

More information

Transforms and Boundary Value Problems

Transforms and Boundary Value Problems Transforms and Boundary Vaue Probems (For B.Tech Students (Third/Fourth/Fifth Semester Soved University Questions Papers Prepared by Dr. V. SUVITHA Department of Mathematics, SRMIST Kattankuathur 6. CONTENTS

More information

A Numerical Method For Constructing Geo-Location Isograms

A Numerical Method For Constructing Geo-Location Isograms A Numerial Method For Construting Geo-Loation Isograms Mike Grabbe The Johns Hopkins University Applied Physis Laboratory Laurel, MD Memo Number GVW--U- June 9, 2 Introdution Geo-loation is often performed

More information

An H 2 type Riemannian metric on the space of planar curves

An H 2 type Riemannian metric on the space of planar curves An H 2 type Riemannian metric on the space of panar curves Jayant hah Mathematics Department, Northeastern University, Boston MA emai: shah@neu.edu Abstract An H 2 type metric on the space of panar curves

More information

New Algorithms for Nonlinear Generalized Disjunctive Programming

New Algorithms for Nonlinear Generalized Disjunctive Programming ew Agorithms for oninear Generaized Disuntive Programming Sangbum Lee and Ignaio E. Grossmann * Department of Chemia Engineering Carnegie Meon University Pittsburgh PA U.S.A. Otober 999 / Marh * To whom

More information

Differential Equations 8/24/2010

Differential Equations 8/24/2010 Differential Equations A Differential i Equation (DE) is an equation ontaining one or more derivatives of an unknown dependant d variable with respet to (wrt) one or more independent variables. Solution

More information

Statistical Mechanics Basis of Macleod s Formula

Statistical Mechanics Basis of Macleod s Formula Preprint Journa of Physia ChemistryB Voume 94, Issue 2, pp.8362-8364, 99 DOI:.2/j384a68 Print ISSN: 22-3654 Eetroni ISSN: 54-574 Mohammed-E. BOUDH-HIR and G.Ai MANSOORI Uniersity of Iinois at Chiago (M/C

More information

VTU-NPTEL-NMEICT Project

VTU-NPTEL-NMEICT Project MODUE-X -CONTINUOUS SYSTEM : APPROXIMATE METHOD VIBRATION ENGINEERING 14 VTU-NPTE-NMEICT Project Progress Report The Project on Deveopment of Remaining Three Quadrants to NPTE Phase-I under grant in aid

More information

The Relationship Between Discrete and Continuous Entropy in EPR-Steering Inequalities. Abstract

The Relationship Between Discrete and Continuous Entropy in EPR-Steering Inequalities. Abstract The Reationship Between Discrete and Continuous Entropy in EPR-Steering Inequaities James Schneeoch 1 1 Department of Physics and Astronomy, University of Rochester, Rochester, NY 14627 arxiv:1312.2604v1

More information

Quantum Mechanical Models of Vibration and Rotation of Molecules Chapter 18

Quantum Mechanical Models of Vibration and Rotation of Molecules Chapter 18 Quantum Mechanica Modes of Vibration and Rotation of Moecues Chapter 18 Moecuar Energy Transationa Vibrationa Rotationa Eectronic Moecuar Motions Vibrations of Moecues: Mode approximates moecues to atoms

More information

Gauss Law. 2. Gauss s Law: connects charge and field 3. Applications of Gauss s Law

Gauss Law. 2. Gauss s Law: connects charge and field 3. Applications of Gauss s Law Gauss Law 1. Review on 1) Couomb s Law (charge and force) 2) Eectric Fied (fied and force) 2. Gauss s Law: connects charge and fied 3. Appications of Gauss s Law Couomb s Law and Eectric Fied Couomb s

More information

Scott Cohen. November 10, Abstract. The method of Block Cyclic Reduction (BCR) is described in the context of

Scott Cohen. November 10, Abstract. The method of Block Cyclic Reduction (BCR) is described in the context of ycic Reduction Scott ohen November, 99 bstract The method of ock ycic Reduction (R) is described in the context of soving Poisson's equation with Dirichet boundary conditions The numerica instabiityof

More information

Supporting Information for Suppressing Klein tunneling in graphene using a one-dimensional array of localized scatterers

Supporting Information for Suppressing Klein tunneling in graphene using a one-dimensional array of localized scatterers Supporting Information for Suppressing Kein tunneing in graphene using a one-dimensiona array of ocaized scatterers Jamie D Was, and Danie Hadad Department of Chemistry, University of Miami, Cora Gabes,

More information

Determining both sound speed and internal source in thermo- and photo-acoustic tomography

Determining both sound speed and internal source in thermo- and photo-acoustic tomography Inverse Problems Inverse Problems (05) 05005 (0pp) doi:0.088/06656//0/05005 Determining both sound speed and internal soure in thermo and photoaousti tomography Hongyu Liu,,5 and Gunther Uhlmann,4 Department

More information

The Second Postulate of Euclid and the Hyperbolic Geometry

The Second Postulate of Euclid and the Hyperbolic Geometry 1 The Seond Postulate of Eulid and the Hyperboli Geometry Yuriy N. Zayko Department of Applied Informatis, Faulty of Publi Administration, Russian Presidential Aademy of National Eonomy and Publi Administration,

More information

ON THE GENERAL QUADRATIC FUNCTIONAL EQUATION

ON THE GENERAL QUADRATIC FUNCTIONAL EQUATION Bol. So. Mat. Mexiana (3) Vol. 11, 2005 ON THE GENERAL QUADRATIC FUNCTIONAL EQUATION JOHN MICHAEL RASSIAS Abstrat. In 1940 and in 1964 S. M. Ulam proposed the general problem: When is it true that by hanging

More information

4 1-D Boundary Value Problems Heat Equation

4 1-D Boundary Value Problems Heat Equation 4 -D Boundary Vaue Probems Heat Equation The main purpose of this chapter is to study boundary vaue probems for the heat equation on a finite rod a x b. u t (x, t = ku xx (x, t, a < x < b, t > u(x, = ϕ(x

More information

A filled function method for constrained global optimization

A filled function method for constrained global optimization DOI 0.007/s0898-007-95- ORIGINAL PAPER A filled funtion method for onstrained global optimization Z. Y. Wu F. S. Bai H. W. J. Lee Y. J. Yang Reeived: 0 Marh 005 / Aepted: 5 February 007 Springer Siene+Business

More information

Relativistic Dynamics

Relativistic Dynamics Chapter 7 Relativisti Dynamis 7.1 General Priniples of Dynamis 7.2 Relativisti Ation As stated in Setion A.2, all of dynamis is derived from the priniple of least ation. Thus it is our hore to find a suitable

More information

Multiple Beam Interference

Multiple Beam Interference MutipeBeamInterference.nb James C. Wyant 1 Mutipe Beam Interference 1. Airy's Formua We wi first derive Airy's formua for the case of no absorption. ü 1.1 Basic refectance and transmittance Refected ight

More information

arxiv: v1 [math-ph] 14 Apr 2008

arxiv: v1 [math-ph] 14 Apr 2008 Inverse Vetor Operators Shaon Sahoo arxiv:0804.9v [math-ph] 4 Apr 008 Department of Physis, Indian Institute of Siene, Bangalore 5600, India. Abstrat In different branhes of physis, we frequently deal

More information

Naïve Bayes for Text Classification

Naïve Bayes for Text Classification Naïve Bayes for Text Cassifiation adapted by Lye Ungar from sides by Mith Marus, whih were adapted from sides by Massimo Poesio, whih were adapted from sides by Chris Manning : Exampe: Is this spam? From:

More information

Strauss PDEs 2e: Section Exercise 3 Page 1 of 13. u tt c 2 u xx = cos x. ( 2 t c 2 2 x)u = cos x. v = ( t c x )u

Strauss PDEs 2e: Section Exercise 3 Page 1 of 13. u tt c 2 u xx = cos x. ( 2 t c 2 2 x)u = cos x. v = ( t c x )u Strauss PDEs e: Setion 3.4 - Exerise 3 Page 1 of 13 Exerise 3 Solve u tt = u xx + os x, u(x, ) = sin x, u t (x, ) = 1 + x. Solution Solution by Operator Fatorization Bring u xx to the other side. Write

More information

MA 201: Partial Differential Equations Lecture - 10

MA 201: Partial Differential Equations Lecture - 10 MA 201: Partia Differentia Equations Lecture - 10 Separation of Variabes, One dimensiona Wave Equation Initia Boundary Vaue Probem (IBVP) Reca: A physica probem governed by a PDE may contain both boundary

More information

RIEMANN S FIRST PROOF OF THE ANALYTIC CONTINUATION OF ζ(s) AND L(s, χ)

RIEMANN S FIRST PROOF OF THE ANALYTIC CONTINUATION OF ζ(s) AND L(s, χ) RIEMANN S FIRST PROOF OF THE ANALYTIC CONTINUATION OF ζ(s AND L(s, χ FELIX RUBIN SEMINAR ON MODULAR FORMS, WINTER TERM 6 Abstrat. In this hapter, we will see a proof of the analyti ontinuation of the Riemann

More information

Complexity of Regularization RBF Networks

Complexity of Regularization RBF Networks Complexity of Regularization RBF Networks Mark A Kon Department of Mathematis and Statistis Boston University Boston, MA 02215 mkon@buedu Leszek Plaskota Institute of Applied Mathematis University of Warsaw

More information

A Queueing Model for Call Blending in Call Centers

A Queueing Model for Call Blending in Call Centers A Queueing Model for Call Blending in Call Centers Sandjai Bhulai and Ger Koole Vrije Universiteit Amsterdam Faulty of Sienes De Boelelaan 1081a 1081 HV Amsterdam The Netherlands E-mail: {sbhulai, koole}@s.vu.nl

More information

Reliability: Theory & Applications No.3, September 2006

Reliability: Theory & Applications No.3, September 2006 REDUNDANCY AND RENEWAL OF SERVERS IN OPENED QUEUING NETWORKS G. Sh. Tsitsiashvii M.A. Osipova Vadivosto, Russia 1 An opened queuing networ with a redundancy and a renewa of servers is considered. To cacuate

More information

Applied Nuclear Physics (Fall 2006) Lecture 7 (10/2/06) Overview of Cross Section Calculation

Applied Nuclear Physics (Fall 2006) Lecture 7 (10/2/06) Overview of Cross Section Calculation 22.101 Appied Nucear Physics (Fa 2006) Lecture 7 (10/2/06) Overview of Cross Section Cacuation References P. Roman, Advanced Quantum Theory (Addison-Wesey, Reading, 1965), Chap 3. A. Foderaro, The Eements

More information

Empty non-convex and convex four-gons in random point sets

Empty non-convex and convex four-gons in random point sets Empty non-convex and convex four-gons in random point sets Ruy Fabia-Monroy 1, Cemens Huemer, and Dieter Mitsche 3 1 Departamento de Matemáticas, CINVESTAV-IPN, México Universitat Poitècnica de Cataunya,

More information

arxiv: v1 [math.fa] 23 Aug 2018

arxiv: v1 [math.fa] 23 Aug 2018 An Exact Upper Bound on the L p Lebesgue Constant and The -Rényi Entropy Power Inequaity for Integer Vaued Random Variabes arxiv:808.0773v [math.fa] 3 Aug 08 Peng Xu, Mokshay Madiman, James Mebourne Abstract

More information

Path planning with PH G2 splines in R2

Path planning with PH G2 splines in R2 Path panning with PH G2 spines in R2 Laurent Gajny, Richard Béarée, Eric Nyiri, Oivier Gibaru To cite this version: Laurent Gajny, Richard Béarée, Eric Nyiri, Oivier Gibaru. Path panning with PH G2 spines

More information

arxiv: v1 [hep-th] 10 Dec 2018

arxiv: v1 [hep-th] 10 Dec 2018 Casimir energy of an open string with ange-dependent boundary condition A. Jahan 1 and I. Brevik 2 1 Research Institute for Astronomy and Astrophysics of Maragha (RIAAM, Maragha, Iran 2 Department of Energy

More information

Green s function for the wave equation

Green s function for the wave equation Green s funtion for the wave equation Non-relativisti ase January 2019 1 The wave equations In the Lorentz Gauge, the wave equations for the potentials are (Notes 1 eqns 43 and 44): 1 2 A 2 2 2 A = µ 0

More information