The Tetrahedron Quality Factors of CSDS

Size: px
Start display at page:

Download "The Tetrahedron Quality Factors of CSDS"

Transcription

1 MAX PLANCK INSTITUT FÜR AERONOMIE D Katlenburg-Lindau, Federal Republi of Germany MPAE W The Tetrahedron Quality Fators of CSDS PATRICK W. DALY 1994 June 7 This report available from Abstrat The four Cluster spaeraft will form a tetrahedron, whih ideally should be a regular one: equal spaing between all pairs of verties. In reality, this will not be the ase. A number of parameters exist to speify how badly off the true figure is. This paper presents some mathematis of tetrahedrons, desribes the two parameters that are to be used in the Cluster Siene Data System, and gives a Fortran program for their alulation. Introdution Four points in spae define a tetrahedron. If the separations between eah pair of points are equal, then it is a regular tetrahedron. The four Cluster spaeraft will form a tetrahedron, whih in general is not regular. How an we speify the degree to whih regularity is ahieved? The Glassmeier Parameter The parameter proposed by vom Stein, Glassmeier, and Dunlop (1992) is defined as Q G = True Vol. True Surf. + Ideal Vol. Ideal Surf. + 1 (1) and takes on values between 1 and 3. It tends to desribe the dimensionality of the figure, as listed in Table 1. The ideal volume and surfae are alulated for a regular tetrahedron with a side length equal to the average of the 6 distanes between the 4 points. Table 1. Speial values of the Glassmeier parameter Q G Meaning 1.0 The four points are olinear 2.0 The points all lie in a plane 3.0 A regular tetrahedron is formed The Robert/Roux Parameter In their paper on tetrahedron shape, Robert and Roux (1993) present 17 different parameters, as ratios of various volumes, sizes, areas. Of these, the CSDS ommunity has deided to adopt one as its seond quality parameter for the auxiliary data. It is defined as ( ) 1 True Vol. 3 Q R = N (2) Sphere Vol. where the sphere is that irumsribing the tetrahedron (all four points on its surfae) and N is a 1

2 2 P. W. DALY normalization fator to make Q R = 1 for a regular tetrahedron. The range of values is between 0 and 1. Mathematis of a Tetrahedron Consider four points in spae and the figure formed by joining them with lines (Figure 1). The points are numbered 0 to 3, and their vetors are r 0, r 1, r 2, r 3. Without any loss of generality, we may onsider only the differenes S d 2 d 1 Figure 2. Area S of a triangle. in desribing the points. Area of a Side d i = r i r 0 The area of a parallelogram bounded by two vetors d 1 and d 2 is given by the magnitude of their ross produt; any triangle is half of a parallelogram, so its area is S = 1 2 d 1 d 2 where d 1 and d 2 are the vetors for any two sides of the triangle (Figure 2). For the four sides of the tetrahedron, speify side n to be that one that does not ontain point n at any of its verties. Thus: S 1 = 1 2 d 2 d 3 (3) S 2 = 1 2 d 1 d 3 (4) Figure 1. A tetrahedron and its four verties. S 3 = 1 2 d 1 d 2 (5) S 0 = 1 2 (d 2 d 1 ) (d 3 d 1 ) = 1 2 d 1 d 2 + d 2 d 3 + d 3 d 1 (6) The total surfae S is the sum 3 n=0 S n. Volume of a Tetrahedron The volume of a figure bounded by three vetors in spae is the triple produt of those vetors. Any tetrahedron is 1/6 of suh a figure, hene V = 1 6 d 1 d 2 d 3 (7) = 1 d 1x d 1y d 1z 6 d 2x d 2y d 2z (8) d 3x d 3y d 3z Center of Cirumsribed Sphere To find the irumsribed sphere, we need the point that is equidistant from all four verties, i.e. we want r suh that (r r n ) (r r n ) = ρ 2 ; n = 0, 3 r 2 2r r n + r 2 n = ρ 2 If we take point 0 as the origin, that is, if we use the d n vetors in plae of the r n, then r 2 = ρ 2, the sphere radius, and the above 4 equations redue to 2r d n = d 2 n ; n = 1, 3

3 THE CSDS TETRAHEDRON FACTORS 3 Table 2. Values for regular tetrahedron Quantity Value S 0 = 3/4 S = 3 V = 2/12 ρ = 6/4 V = 4 3 π ( 3 8 This yields the matrix equation for the enter of the sphere d 1x d 1y d 1z x d d 2x d 2y d 2z y = d 2 2 (9) d 3x d 3y d 3z z whih an be solved for the vetor (x, y, z) and the radius of the sphere ρ 2 = x 2 +y 2 +z 2. Note that the leftmost matrix in equation 9 is the same as the one whose determinant yields the volume of the tetrahedron (equation 8). The volume of the irumsribed sphere is then ) 3 2 d 2 3 V = 4 3 πρ2 (10) The Regular Tetrahedron The regular tetrahedron of unit side is the ideal against whih the true figure of the four spaeraft is to be measured. We may take d 0 = (0, 0, 0) d 1 = (1, 0, 0) ( ) 1 3 d 2 = 2, 2, 0 ( ) d 3 = 2, 6, 3 Values for the regular tetrahedron of unit side length are listed in Table 2. Calulating the Quality Fators The quality fators in equations 1 and 2 an now be found with the help of these formulas. For Q G, we average the 6 distanes between the 4 points to get the side L of the ideal regular tetrahedron, with volume L 3 2/12 and surfae L 2 3. The true volume and surfae are found from equations 7 and 3 6. For Q R, the radius of the irumsribing sphere is alulated from equation 9. The atual volume of the sphere need not be alulated, for all the fators just go into the normalizing N. Q R = ( 9 ) V ρ 1 A Fortran program at the end of this paper alulates both these parameters. Referenes Robert, P. and Roux, A. (1993). Influene of the Shape of the Tetrahedron on the Auray of the Estimate of the Current Density. Proeedings of ESA START Conferene, Aussois, Frane, Centre de Reherhes en Physique de l Environment, Issy les Moulineaux, Frane. vom Stein, R., Glassmeier, K.-H., and Dunlop, M. (1992). A Configuration Parameter for the Cluster Satellites. Teh. Rep. 2/1992, Institut für Geophysik und Meteologie der Tehnishen Universität Braunshweig.

4 4 P. W. DALY A Fortran Subroutine to Calulate the Parameters subroutine TETRAQ(r,qg,qr) To alulate the Glassmeier (QG) and Robert/Roux (QR) quality fators for a tetrahedron. Appliation: CLUSTER SCIENCE DATA SYSTEM (These are to be two auxiliary parameters) Input: R(3,4) = positions of the 4 points Output: QG = Glassmeier fator QR = Robert/Roux fator (their fator number 10) Inputs and outputs are single preision, internal alulations are double preision True volume True surfae QG = Ideal vol Ideal surf where the ideals are volume and surfae of a regular tetrahedron of side length equal to the mean of the 6 sides. True volume (1/3) QR = Fator * Sphere vol where the sphere is that irumsribing the tetrahedron (all 4 points on the surfae), and the fator is suh that QR=1 for a regular tetrahedron. ********************************************************************* Patrik W. Daly daly@linmpi.mpg.de Max-Plank-Institut fuer Aeronomie D Katlenburg-Lindau Germany 1994 June 7 ********************************************************************* impliit none real r(3,4),qg,qr double preision d(3,3),(3,3),s1,s2,s3,s0,s,l1,l2,l3,vol double preision v(3),w,smean,vmean,lmean,r double preision dot integer n,m,k Find the differenes w=dble(r(n,1)) do m=1,3

5 THE CSDS TETRAHEDRON FACTORS 5 d(n,m)=dble(r(n,m+1))-w Find the average side length of all 6 sides l1=dsqrt(dot(d(1,1),d(1,1))) l2=dsqrt(dot(d(1,2),d(1,2))) l3=dsqrt(dot(d(1,3),d(1,3))) w= l1 + l2 + l3 v(n)=d(n,2)-d(n,1) w=w + dsqrt(dot(v,v)) v(n)=d(n,3)-d(n,1) w=w + dsqrt(dot(v,v)) v(n)=d(n,3)-d(n,2) w=w + dsqrt(dot(v,v)) lmean=w/6.d0 Find the ross produts m=mod(n,3) + 1 k=mod(m,3) + 1 all ross(d(1,m),d(1,k),(1,n)) Find the volume of the tetrahedron vol=dabs(dot(d(1,1),(1,1)))/6.d0 Find the area of the 4 surfaes and their sum s1=0.5d0*dsqrt(dot((1,1),(1,1))) s2=0.5d0*dsqrt(dot((1,2),(1,2))) s3=0.5d0*dsqrt(dot((1,3),(1,3))) v(n)=(n,1) + (n,2) + (n,3) s0=0.5d0*dsqrt(dot(v,v)) s=s0 + s1 + s2 + s3 Find the volume and total area for reg tetrahedron with mean side vmean=dsqrt(2.d0)*lmean*lmean*lmean/1.2d1 smean=dsqrt(3.d0)*lmean*lmean

6 6 P. W. DALY Calulate the Glassmeier fator w= vol/vmean + s/smean + 1.d0 qg=sngl(w) Find the enter of the irumsribed irle w=1.d0/(1.2d1*vol) v(1)=w*((1,1)*l1*l1 + (1,2)*l2*l2 + (1,3)*l3*l3) v(2)=w*((2,1)*l1*l1 + (2,2)*l2*l2 + (2,3)*l3*l3) v(3)=w*((3,1)*l1*l1 + (3,2)*l2*l2 + (3,3)*l3*l3) r=dsqrt(dot(v,v)) Calulate the Robert/Roux fator w=9.d0*dsqrt(3.d0)/8.d0 w=(w*vol)**(1.d0/3.d0)/r qr=sngl(w) return end funtion DOT(v,w) To return the dot produt of vetors V and W impliit none double preision dot,v(3),w(3) dot=v(1)*w(1) + v(2)*w(2) + v(3)*w(3) return end subroutine CROSS(v,w,x) To return X as the ross produt of vetors V and W impliit none double preision x(3),w(3),v(3) x(1)=v(2)*w(3) - v(3)*w(2) x(2)=v(3)*w(1) - v(1)*w(3) x(3)=v(1)*w(2) - v(2)*w(1) return end

COMBINED PROBE FOR MACH NUMBER, TEMPERATURE AND INCIDENCE INDICATION

COMBINED PROBE FOR MACH NUMBER, TEMPERATURE AND INCIDENCE INDICATION 4 TH INTERNATIONAL CONGRESS OF THE AERONAUTICAL SCIENCES COMBINED PROBE FOR MACH NUMBER, TEMPERATURE AND INCIDENCE INDICATION Jiri Nozika*, Josef Adame*, Daniel Hanus** *Department of Fluid Dynamis and

More information

F = F x x + F y. y + F z

F = F x x + F y. y + F z ECTION 6: etor Calulus MATH20411 You met vetors in the first year. etor alulus is essentially alulus on vetors. We will need to differentiate vetors and perform integrals involving vetors. In partiular,

More information

HIGHER SECONDARY FIRST YEAR MATHEMATICS

HIGHER SECONDARY FIRST YEAR MATHEMATICS HIGHER SECONDARY FIRST YEAR MATHEMATICS ANALYTICAL GEOMETRY Creative Questions Time :.5 Hrs Marks : 45 Part - I Choose the orret answer 0 = 0. The angle between the straight lines 4y y 0 is a) 0 30 b)

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

arxiv:math/ v1 [math.ca] 27 Nov 2003

arxiv:math/ v1 [math.ca] 27 Nov 2003 arxiv:math/011510v1 [math.ca] 27 Nov 200 Counting Integral Lamé Equations by Means of Dessins d Enfants Sander Dahmen November 27, 200 Abstrat We obtain an expliit formula for the number of Lamé equations

More information

Q2. [40 points] Bishop-Hill Model: Calculation of Taylor Factors for Multiple Slip

Q2. [40 points] Bishop-Hill Model: Calculation of Taylor Factors for Multiple Slip 27-750, A.D. Rollett Due: 20 th Ot., 2011. Homework 5, Volume Frations, Single and Multiple Slip Crystal Plastiity Note the 2 extra redit questions (at the end). Q1. [40 points] Single Slip: Calulating

More information

Developing Excel Macros for Solving Heat Diffusion Problems

Developing Excel Macros for Solving Heat Diffusion Problems Session 50 Developing Exel Maros for Solving Heat Diffusion Problems N. N. Sarker and M. A. Ketkar Department of Engineering Tehnology Prairie View A&M University Prairie View, TX 77446 Abstrat This paper

More information

THE TWIN PARADOX A RELATIVISTIC DOMAIN RESOLUTION

THE TWIN PARADOX A RELATIVISTIC DOMAIN RESOLUTION THE TWIN PARADOX A RELATIVISTIC DOMAIN RESOLUTION Peter G.Bass P.G.Bass www.relativitydomains.om January 0 ABSTRACT This short paper shows that the so alled "Twin Paradox" of Speial Relativity, is in fat

More information

The Effectiveness of the Linear Hull Effect

The Effectiveness of the Linear Hull Effect The Effetiveness of the Linear Hull Effet S. Murphy Tehnial Report RHUL MA 009 9 6 Otober 009 Department of Mathematis Royal Holloway, University of London Egham, Surrey TW0 0EX, England http://www.rhul.a.uk/mathematis/tehreports

More information

Lecture 3 - Lorentz Transformations

Lecture 3 - Lorentz Transformations Leture - Lorentz Transformations A Puzzle... Example A ruler is positioned perpendiular to a wall. A stik of length L flies by at speed v. It travels in front of the ruler, so that it obsures part of the

More information

Discrete Bessel functions and partial difference equations

Discrete Bessel functions and partial difference equations Disrete Bessel funtions and partial differene equations Antonín Slavík Charles University, Faulty of Mathematis and Physis, Sokolovská 83, 186 75 Praha 8, Czeh Republi E-mail: slavik@karlin.mff.uni.z Abstrat

More information

Hankel Optimal Model Order Reduction 1

Hankel Optimal Model Order Reduction 1 Massahusetts Institute of Tehnology Department of Eletrial Engineering and Computer Siene 6.245: MULTIVARIABLE CONTROL SYSTEMS by A. Megretski Hankel Optimal Model Order Redution 1 This leture overs both

More information

c-perfect Hashing Schemes for Binary Trees, with Applications to Parallel Memories

c-perfect Hashing Schemes for Binary Trees, with Applications to Parallel Memories -Perfet Hashing Shemes for Binary Trees, with Appliations to Parallel Memories (Extended Abstrat Gennaro Cordaso 1, Alberto Negro 1, Vittorio Sarano 1, and Arnold L.Rosenberg 2 1 Dipartimento di Informatia

More information

Singular Event Detection

Singular Event Detection Singular Event Detetion Rafael S. Garía Eletrial Engineering University of Puerto Rio at Mayagüez Rafael.Garia@ee.uprm.edu Faulty Mentor: S. Shankar Sastry Researh Supervisor: Jonathan Sprinkle Graduate

More information

Chapter 9. The excitation process

Chapter 9. The excitation process Chapter 9 The exitation proess qualitative explanation of the formation of negative ion states Ne and He in He-Ne ollisions an be given by using a state orrelation diagram. state orrelation diagram is

More information

COMPARISON OF COASTAL FLOODING PROBABILITY CALCULATION MODELS FOR FLOOD DEFENCES

COMPARISON OF COASTAL FLOODING PROBABILITY CALCULATION MODELS FOR FLOOD DEFENCES COMPARISON OF COASTAL FLOODING PROBABILITY CALCULATION MODELS FOR FLOOD DEFENCES Elisabet de Boer 1, Andreas Kortenhaus 2 and Pieter van Gelder 3 Reliability alulations for oastal flood defene systems

More information

The universal model of error of active power measuring channel

The universal model of error of active power measuring channel 7 th Symposium EKO TC 4 3 rd Symposium EKO TC 9 and 5 th WADC Workshop nstrumentation for the CT Era Sept. 8-2 Kosie Slovakia The universal model of error of ative power measuring hannel Boris Stogny Evgeny

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

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

Maximum Entropy and Exponential Families

Maximum Entropy and Exponential Families Maximum Entropy and Exponential Families April 9, 209 Abstrat The goal of this note is to derive the exponential form of probability distribution from more basi onsiderations, in partiular Entropy. It

More information

CMSC 451: Lecture 9 Greedy Approximation: Set Cover Thursday, Sep 28, 2017

CMSC 451: Lecture 9 Greedy Approximation: Set Cover Thursday, Sep 28, 2017 CMSC 451: Leture 9 Greedy Approximation: Set Cover Thursday, Sep 28, 2017 Reading: Chapt 11 of KT and Set 54 of DPV Set Cover: An important lass of optimization problems involves overing a ertain domain,

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

Grasp Planning: How to Choose a Suitable Task Wrench Space

Grasp Planning: How to Choose a Suitable Task Wrench Space Grasp Planning: How to Choose a Suitable Task Wrenh Spae Ch. Borst, M. Fisher and G. Hirzinger German Aerospae Center - DLR Institute for Robotis and Mehatronis 8223 Wessling, Germany Email: [Christoph.Borst,

More information

REFINED UPPER BOUNDS FOR THE LINEAR DIOPHANTINE PROBLEM OF FROBENIUS. 1. Introduction

REFINED UPPER BOUNDS FOR THE LINEAR DIOPHANTINE PROBLEM OF FROBENIUS. 1. Introduction Version of 5/2/2003 To appear in Advanes in Applied Mathematis REFINED UPPER BOUNDS FOR THE LINEAR DIOPHANTINE PROBLEM OF FROBENIUS MATTHIAS BECK AND SHELEMYAHU ZACKS Abstrat We study the Frobenius problem:

More information

Likelihood-confidence intervals for quantiles in Extreme Value Distributions

Likelihood-confidence intervals for quantiles in Extreme Value Distributions Likelihood-onfidene intervals for quantiles in Extreme Value Distributions A. Bolívar, E. Díaz-Franés, J. Ortega, and E. Vilhis. Centro de Investigaión en Matemátias; A.P. 42, Guanajuato, Gto. 36; Méxio

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

Array Design for Superresolution Direction-Finding Algorithms

Array Design for Superresolution Direction-Finding Algorithms Array Design for Superresolution Diretion-Finding Algorithms Naushad Hussein Dowlut BEng, ACGI, AMIEE Athanassios Manikas PhD, DIC, AMIEE, MIEEE Department of Eletrial Eletroni Engineering Imperial College

More information

After the completion of this section the student should recall

After the completion of this section the student should recall Chapter I MTH FUNDMENTLS I. Sets, Numbers, Coordinates, Funtions ugust 30, 08 3 I. SETS, NUMERS, COORDINTES, FUNCTIONS Objetives: fter the ompletion of this setion the student should reall - the definition

More information

Error Bounds for Context Reduction and Feature Omission

Error Bounds for Context Reduction and Feature Omission Error Bounds for Context Redution and Feature Omission Eugen Bek, Ralf Shlüter, Hermann Ney,2 Human Language Tehnology and Pattern Reognition, Computer Siene Department RWTH Aahen University, Ahornstr.

More information

Velocity Addition in Space/Time David Barwacz 4/23/

Velocity Addition in Space/Time David Barwacz 4/23/ Veloity Addition in Spae/Time 003 David arwaz 4/3/003 daveb@triton.net http://members.triton.net/daveb Abstrat Using the spae/time geometry developed in the previous paper ( Non-orthogonal Spae- Time geometry,

More information

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion Millennium Relativity Aeleration Composition he Relativisti Relationship between Aeleration and niform Motion Copyright 003 Joseph A. Rybzyk Abstrat he relativisti priniples developed throughout the six

More information

Applying CIECAM02 for Mobile Display Viewing Conditions

Applying CIECAM02 for Mobile Display Viewing Conditions Applying CIECAM2 for Mobile Display Viewing Conditions YungKyung Park*, ChangJun Li*, M.. Luo*, Youngshin Kwak**, Du-Sik Park **, and Changyeong Kim**; * University of Leeds, Colour Imaging Lab, UK*, **

More information

7.1 Roots of a Polynomial

7.1 Roots of a Polynomial 7.1 Roots of a Polynomial A. Purpose Given the oeffiients a i of a polynomial of degree n = NDEG > 0, a 1 z n + a 2 z n 1 +... + a n z + a n+1 with a 1 0, this subroutine omputes the NDEG roots of the

More information

Critical Reflections on the Hafele and Keating Experiment

Critical Reflections on the Hafele and Keating Experiment Critial Refletions on the Hafele and Keating Experiment W.Nawrot In 1971 Hafele and Keating performed their famous experiment whih onfirmed the time dilation predited by SRT by use of marosopi loks. As

More information

SHIELDING MATERIALS FOR HIGH-ENERGY NEUTRONS

SHIELDING MATERIALS FOR HIGH-ENERGY NEUTRONS SHELDNG MATERALS FOR HGH-ENERGY NEUTRONS Hsiao-Hua Hsu Health Physis Measurements Group Los Alamos National Laboratory Los Alamos, New Mexio, 87545 USA Abstrat We used the Monte Carlo transport ode Los

More information

The gravitational phenomena without the curved spacetime

The gravitational phenomena without the curved spacetime The gravitational phenomena without the urved spaetime Mirosław J. Kubiak Abstrat: In this paper was presented a desription of the gravitational phenomena in the new medium, different than the urved spaetime,

More information

Espen Gaarder Haug Norwegian University of Life Sciences April 4, 2017

Espen Gaarder Haug Norwegian University of Life Sciences April 4, 2017 The Mass Gap, Kg, the Plank Constant and the Gravity Gap The Plank Constant Is a Composite Constant One kg Is 85465435748 0 36 Collisions per Seond The Mass Gap Is.734 0 5 kg and also m p The Possibility

More information

Name Solutions to Test 1 September 23, 2016

Name Solutions to Test 1 September 23, 2016 Name Solutions to Test 1 September 3, 016 This test onsists of three parts. Please note that in parts II and III, you an skip one question of those offered. Possibly useful formulas: F qequb x xvt E Evpx

More information

Pseudo Spheres. A Sample of Electronic Lecture Notes in Mathematics. Eberhard Malkowsky.

Pseudo Spheres. A Sample of Electronic Lecture Notes in Mathematics. Eberhard Malkowsky. Pseudo Spheres A Sample of Eletroni Leture Notes in Mathematis Eberhard Malkowsky Mathematishes Institut Justus Liebig Universität Gießen Arndtstraße D-3539 Gießen Germany /o Shool of Informatis Computing

More information

Measuring & Inducing Neural Activity Using Extracellular Fields I: Inverse systems approach

Measuring & Inducing Neural Activity Using Extracellular Fields I: Inverse systems approach Measuring & Induing Neural Ativity Using Extraellular Fields I: Inverse systems approah Keith Dillon Department of Eletrial and Computer Engineering University of California San Diego 9500 Gilman Dr. La

More information

A Recursive Approach to the Kauffman Bracket

A Recursive Approach to the Kauffman Bracket Applied Mathematis, 204, 5, 2746-2755 Published Online Otober 204 in SiRes http://wwwsirporg/journal/am http://ddoiorg/04236/am20457262 A Reursive Approah to the Kauffman Braet Abdul Rauf Nizami, Mobeen

More information

(c) Calculate the tensile yield stress based on a critical resolved shear stress that we will (arbitrarily) set at 100 MPa. (c) MPa.

(c) Calculate the tensile yield stress based on a critical resolved shear stress that we will (arbitrarily) set at 100 MPa. (c) MPa. 27-750, A.D. Rollett Due: 20 th Ot., 2011. Homework 5, Volume Frations, Single and Multiple Slip Crystal Plastiity Note the 2 extra redit questions (at the end). Q1. [40 points] Single Slip: Calulating

More information

MODELING MATTER AT NANOSCALES. 4. Introduction to quantum treatments Eigenvectors and eigenvalues of a matrix

MODELING MATTER AT NANOSCALES. 4. Introduction to quantum treatments Eigenvectors and eigenvalues of a matrix MODELING MATTER AT NANOSCALES 4 Introdution to quantum treatments 403 Eigenvetors and eigenvalues of a matrix Simultaneous equations in the variational method The problem of simultaneous equations in the

More information

The First Principle of Thermodynamics under Relativistic Conditions and Temperature

The First Principle of Thermodynamics under Relativistic Conditions and Temperature New Horizons in Mathematial Physis, Vol., No., September 7 https://dx.doi.org/.66/nhmp.7. 37 he First Priniple of hermodynamis under Relativisti Conditions and emperature Emil Veitsman Independent Researher

More information

12 th Maths Way to Success

12 th Maths Way to Success th Maths Quarterly Eam-7-Answer Key Part - A Q.No Option Q.No Option Q.No Option Q.No Option 6 6 6 6 7 7 7 7 8 8 8 8 9 9 9 9 Part B. A adj A A adja..() adja A () A I () From (), (),() we get A adja adja

More information

Danielle Maddix AA238 Final Project December 9, 2016

Danielle Maddix AA238 Final Project December 9, 2016 Struture and Parameter Learning in Bayesian Networks with Appliations to Prediting Breast Caner Tumor Malignany in a Lower Dimension Feature Spae Danielle Maddix AA238 Final Projet Deember 9, 2016 Abstrat

More information

Design and Development of Three Stages Mixed Sampling Plans for Variable Attribute Variable Quality Characteristics

Design and Development of Three Stages Mixed Sampling Plans for Variable Attribute Variable Quality Characteristics International Journal of Statistis and Systems ISSN 0973-2675 Volume 12, Number 4 (2017), pp. 763-772 Researh India Publiations http://www.ripubliation.om Design and Development of Three Stages Mixed Sampling

More information

Simple Considerations on the Cosmological Redshift

Simple Considerations on the Cosmological Redshift Apeiron, Vol. 5, No. 3, July 8 35 Simple Considerations on the Cosmologial Redshift José Franiso Garía Juliá C/ Dr. Maro Mereniano, 65, 5. 465 Valenia (Spain) E-mail: jose.garia@dival.es Generally, the

More information

Rigorous prediction of quadratic hyperchaotic attractors of the plane

Rigorous prediction of quadratic hyperchaotic attractors of the plane Rigorous predition of quadrati hyperhaoti attrators of the plane Zeraoulia Elhadj 1, J. C. Sprott 2 1 Department of Mathematis, University of Tébéssa, 12000), Algeria. E-mail: zeraoulia@mail.univ-tebessa.dz

More information

INTRO VIDEOS. LESSON 9.5: The Doppler Effect

INTRO VIDEOS. LESSON 9.5: The Doppler Effect DEVIL PHYSICS BADDEST CLASS ON CAMPUS IB PHYSICS INTRO VIDEOS Big Bang Theory of the Doppler Effet Doppler Effet LESSON 9.5: The Doppler Effet 1. Essential Idea: The Doppler Effet desribes the phenomenon

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

Exercise 3: Quadratic sequences

Exercise 3: Quadratic sequences Exerise 3: s Problem 1: Determine whether eah of the following sequenes is: a linear sequene; a quadrati sequene; or neither.. 3. 4. 5. 6. 7. 8. 8;17;3;53;80; 3 p ;6 p ;9 p ;1 p ;15 p ; 1;,5;5;8,5;13;

More information

Relative Maxima and Minima sections 4.3

Relative Maxima and Minima sections 4.3 Relative Maxima and Minima setions 4.3 Definition. By a ritial point of a funtion f we mean a point x 0 in the domain at whih either the derivative is zero or it does not exists. So, geometrially, one

More information

Packing Plane Spanning Trees into a Point Set

Packing Plane Spanning Trees into a Point Set Paking Plane Spanning Trees into a Point Set Ahmad Biniaz Alfredo Garía Abstrat Let P be a set of n points in the plane in general position. We show that at least n/3 plane spanning trees an be paked into

More information

MASSACHUSETTS MATHEMATICS LEAGUE CONTEST 3 DECEMBER 2013 ROUND 1 TRIG: RIGHT ANGLE PROBLEMS, LAWS OF SINES AND COSINES

MASSACHUSETTS MATHEMATICS LEAGUE CONTEST 3 DECEMBER 2013 ROUND 1 TRIG: RIGHT ANGLE PROBLEMS, LAWS OF SINES AND COSINES CONTEST 3 DECEMBER 03 ROUND TRIG: RIGHT ANGLE PROBLEMS, LAWS OF SINES AND COSINES ANSWERS A) B) C) A) The sides of right ΔABC are, and 7, where < < 7. A is the larger aute angle. Compute the tan( A). B)

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

MATHEMATICAL AND NUMERICAL BASIS OF BINARY ALLOY SOLIDIFICATION MODELS WITH SUBSTITUTE THERMAL CAPACITY. PART II

MATHEMATICAL AND NUMERICAL BASIS OF BINARY ALLOY SOLIDIFICATION MODELS WITH SUBSTITUTE THERMAL CAPACITY. PART II Journal of Applied Mathematis and Computational Mehanis 2014, 13(2), 141-147 MATHEMATICA AND NUMERICA BAI OF BINARY AOY OIDIFICATION MODE WITH UBTITUTE THERMA CAPACITY. PART II Ewa Węgrzyn-krzypzak 1,

More information

Nonreversibility of Multiple Unicast Networks

Nonreversibility of Multiple Unicast Networks Nonreversibility of Multiple Uniast Networks Randall Dougherty and Kenneth Zeger September 27, 2005 Abstrat We prove that for any finite direted ayli network, there exists a orresponding multiple uniast

More information

EINSTEIN FIELD EQUATIONS OBTAINED ONLY WITH GAUSS CURVATURE AND ZOOM UNIVERSE MODEL CHARACTERISTICS

EINSTEIN FIELD EQUATIONS OBTAINED ONLY WITH GAUSS CURVATURE AND ZOOM UNIVERSE MODEL CHARACTERISTICS EINSTEIN FIELD EQUATIONS OBTAINED ONLY WITH GAUSS CURVATURE AND ZOOM UNIVERSE MODEL CHARACTERISTICS Sergio Garia Chimeno Abstrat Demonstration how to obtain the Einstein Field Equations without using the

More information

Phys 561 Classical Electrodynamics. Midterm

Phys 561 Classical Electrodynamics. Midterm Phys 56 Classial Eletrodynamis Midterm Taner Akgün Department of Astronomy and Spae Sienes Cornell University Otober 3, Problem An eletri dipole of dipole moment p, fixed in diretion, is loated at a position

More information

Weighted K-Nearest Neighbor Revisited

Weighted K-Nearest Neighbor Revisited Weighted -Nearest Neighbor Revisited M. Biego University of Verona Verona, Italy Email: manuele.biego@univr.it M. Loog Delft University of Tehnology Delft, The Netherlands Email: m.loog@tudelft.nl Abstrat

More information

A Variational Definition for Limit and Derivative

A Variational Definition for Limit and Derivative Amerian Journal of Applied Mathematis 2016; 4(3): 137-141 http://www.sienepublishinggroup.om/j/ajam doi: 10.11648/j.ajam.20160403.14 ISSN: 2330-0043 (Print); ISSN: 2330-006X (Online) A Variational Definition

More information

Theory. Coupled Rooms

Theory. Coupled Rooms Theory of Coupled Rooms For: nternal only Report No.: R/50/TCR Prepared by:. N. taey B.., MO Otober 00 .00 Objet.. The objet of this doument is present the theory alulations to estimate the reverberant

More information

SERIJA III

SERIJA III SERIJA III www.math.hr/glasnik I. Gaál, B. Jadrijević and L. Remete Totally real Thue inequalities over imaginary quadrati fields Aepted manusript This is a preliminary PDF of the author-produed manusript

More information

The Possibility of FTL Space Travel by using the Quantum Tunneling Effect through the Light Barrier

The Possibility of FTL Space Travel by using the Quantum Tunneling Effect through the Light Barrier ISSN: 19-98 The Possibility of FTL Spae Travel by using the Quantum Tunneling Effet through the Light Barrier Musha T Advaned Si-Teh Researh Organization, -11-7-61, Namiki, Kanazawa-Ku, Yokohama 65, Japan

More information

Fiber Optic Cable Transmission Losses with Perturbation Effects

Fiber Optic Cable Transmission Losses with Perturbation Effects Fiber Opti Cable Transmission Losses with Perturbation Effets Kampanat Namngam 1*, Preeha Yupapin 2 and Pakkinee Chitsakul 1 1 Department of Mathematis and Computer Siene, Faulty of Siene, King Mongkut

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

An Adaptive Optimization Approach to Active Cancellation of Repeated Transient Vibration Disturbances

An Adaptive Optimization Approach to Active Cancellation of Repeated Transient Vibration Disturbances An aptive Optimization Approah to Ative Canellation of Repeated Transient Vibration Disturbanes David L. Bowen RH Lyon Corp / Aenteh, 33 Moulton St., Cambridge, MA 138, U.S.A., owen@lyonorp.om J. Gregory

More information

Green s Function for Potential Field Extrapolation

Green s Function for Potential Field Extrapolation Green s Funtion for Potential Field Extrapolation. Soe Preliinaries on the Potential Magneti Field By definition, a potential agneti field is one for whih the eletri urrent density vanishes. That is, J

More information

Einstein s Three Mistakes in Special Relativity Revealed. Copyright Joseph A. Rybczyk

Einstein s Three Mistakes in Special Relativity Revealed. Copyright Joseph A. Rybczyk Einstein s Three Mistakes in Speial Relativity Revealed Copyright Joseph A. Rybzyk Abstrat When the evidene supported priniples of eletromagneti propagation are properly applied, the derived theory is

More information

Relativistic effects in earth-orbiting Doppler lidar return signals

Relativistic effects in earth-orbiting Doppler lidar return signals 3530 J. Opt. So. Am. A/ Vol. 4, No. 11/ November 007 Neil Ashby Relativisti effets in earth-orbiting Doppler lidar return signals Neil Ashby 1,, * 1 Department of Physis, University of Colorado, Boulder,

More information

Advances in Radio Science

Advances in Radio Science Advanes in adio Siene 2003) 1: 99 104 Copernius GmbH 2003 Advanes in adio Siene A hybrid method ombining the FDTD and a time domain boundary-integral equation marhing-on-in-time algorithm A Beker and V

More information

Ordered fields and the ultrafilter theorem

Ordered fields and the ultrafilter theorem F U N D A M E N T A MATHEMATICAE 59 (999) Ordered fields and the ultrafilter theorem by R. B e r r (Dortmund), F. D e l o n (Paris) and J. S h m i d (Dortmund) Abstrat. We prove that on the basis of ZF

More information

Sufficient Conditions for a Flexible Manufacturing System to be Deadlocked

Sufficient Conditions for a Flexible Manufacturing System to be Deadlocked Paper 0, INT 0 Suffiient Conditions for a Flexile Manufaturing System to e Deadloked Paul E Deering, PhD Department of Engineering Tehnology and Management Ohio University deering@ohioedu Astrat In reent

More information

Collinear Equilibrium Points in the Relativistic R3BP when the Bigger Primary is a Triaxial Rigid Body Nakone Bello 1,a and Aminu Abubakar Hussain 2,b

Collinear Equilibrium Points in the Relativistic R3BP when the Bigger Primary is a Triaxial Rigid Body Nakone Bello 1,a and Aminu Abubakar Hussain 2,b International Frontier Siene Letters Submitted: 6-- ISSN: 9-8, Vol., pp -6 Aepted: -- doi:.8/www.sipress.om/ifsl.. Online: --8 SiPress Ltd., Switzerland Collinear Equilibrium Points in the Relativisti

More information

Heat exchangers: Heat exchanger types:

Heat exchangers: Heat exchanger types: Heat exhangers: he proess of heat exhange between two fluids that are at different temperatures and separated by a solid wall ours in many engineering appliations. he devie used to implement this exhange

More information

Control Theory association of mathematics and engineering

Control Theory association of mathematics and engineering Control Theory assoiation of mathematis and engineering Wojieh Mitkowski Krzysztof Oprzedkiewiz Department of Automatis AGH Univ. of Siene & Tehnology, Craow, Poland, Abstrat In this paper a methodology

More information

Introduction to Exergoeconomic and Exergoenvironmental Analyses

Introduction to Exergoeconomic and Exergoenvironmental Analyses Tehnishe Universität Berlin Introdution to Exergoeonomi and Exergoenvironmental Analyses George Tsatsaronis The Summer Course on Exergy and its Appliation for Better Environment Oshawa, Canada April, 30

More information

Homework Set 4. gas B open end

Homework Set 4. gas B open end Homework Set 4 (1). A steady-state Arnold ell is used to determine the diffusivity of toluene (speies A) in air (speies B) at 298 K and 1 atm. If the diffusivity is DAB = 0.0844 m 2 /s = 8.44 x 10-6 m

More information

SURFACE WAVES OF NON-RAYLEIGH TYPE

SURFACE WAVES OF NON-RAYLEIGH TYPE SURFACE WAVES OF NON-RAYLEIGH TYPE by SERGEY V. KUZNETSOV Institute for Problems in Mehanis Prosp. Vernadskogo, 0, Mosow, 75 Russia e-mail: sv@kuznetsov.msk.ru Abstrat. Existene of surfae waves of non-rayleigh

More information

Q.B.- Maths I + II - FYJC - Ver

Q.B.- Maths I + II - FYJC - Ver Q.B.- Maths I + II - FYJC - Ver -709 Q Find the equation of lous of a point, whih moves suh that the ratio of its distanes from (,0) and (, ) is :. ( : 9x + 9y + x - 0y + 86 0) Q Q Find the equation of

More information

Calculation of Magnetic Field of Two Coaxially Located Circular Permanent Magnets Using a Method of Physical Analogies

Calculation of Magnetic Field of Two Coaxially Located Circular Permanent Magnets Using a Method of Physical Analogies World Applied Sienes Journal 3 (): 345-35, 3 ISSN 88-495 IDOSI Puliations, 3 DOI: 589/idosiwasj3335 Calulation of Magneti Field of Two Coaxially Loated Cirular Permanent Magnets Using a Method of Physial

More information

V. Interacting Particles

V. Interacting Particles V. Interating Partiles V.A The Cumulant Expansion The examples studied in the previous setion involve non-interating partiles. It is preisely the lak of interations that renders these problems exatly solvable.

More information

The transition between quasi-static and fully dynamic for interfaces

The transition between quasi-static and fully dynamic for interfaces Physia D 198 (24) 136 147 The transition between quasi-stati and fully dynami for interfaes G. Caginalp, H. Merdan Department of Mathematis, University of Pittsburgh, Pittsburgh, PA 1526, USA Reeived 6

More information

Lyapunov Exponents of Second Order Linear Systems

Lyapunov Exponents of Second Order Linear Systems Reent Researhes in Computational Intelligene and Information Seurity Lyapunov Exponents of Seond Order Linear Systems ADAM CZORNIK and ALEKSANDER NAWRAT Department of Automati Control Silesian Tehnial

More information

UTC. Engineering 329. Proportional Controller Design. Speed System. John Beverly. Green Team. John Beverly Keith Skiles John Barker.

UTC. Engineering 329. Proportional Controller Design. Speed System. John Beverly. Green Team. John Beverly Keith Skiles John Barker. UTC Engineering 329 Proportional Controller Design for Speed System By John Beverly Green Team John Beverly Keith Skiles John Barker 24 Mar 2006 Introdution This experiment is intended test the variable

More information

Remarks Around Lorentz Transformation

Remarks Around Lorentz Transformation Remarks Around Lorentz Transformation Arm Boris Nima arm.boris@gmail.om Abstrat After diagonalizing the Lorentz Matrix, we find the frame where the Dira equation is one derivation and we alulate the speed

More information

The Lorenz Transform

The Lorenz Transform The Lorenz Transform Flameno Chuk Keyser Part I The Einstein/Bergmann deriation of the Lorentz Transform I follow the deriation of the Lorentz Transform, following Peter S Bergmann in Introdution to the

More information

Fuzzy inner product space and its properties 1

Fuzzy inner product space and its properties 1 International Journal of Fuzzy Mathematis and Systems IJFMS). ISSN 48-9940 Volume 5, Number 1 015), pp. 57-69 Researh India Publiations http://www.ripubliation.om Fuzzy inner produt spae and its properties

More information

Wavetech, LLC. Ultrafast Pulses and GVD. John O Hara Created: Dec. 6, 2013

Wavetech, LLC. Ultrafast Pulses and GVD. John O Hara Created: Dec. 6, 2013 Ultrafast Pulses and GVD John O Hara Created: De. 6, 3 Introdution This doument overs the basi onepts of group veloity dispersion (GVD) and ultrafast pulse propagation in an optial fiber. Neessarily, it

More information

A simple expression for radial distribution functions of pure fluids and mixtures

A simple expression for radial distribution functions of pure fluids and mixtures A simple expression for radial distribution funtions of pure fluids and mixtures Enrio Matteoli a) Istituto di Chimia Quantistia ed Energetia Moleolare, CNR, Via Risorgimento, 35, 56126 Pisa, Italy G.

More information

General solution to a higher-order linear difference equation and existence of bounded solutions

General solution to a higher-order linear difference equation and existence of bounded solutions Stević Advanes in Differene Equations 2017 2017:377 DOI 101186/s13662-017-1432-7 R E S E A R C H Open Aess General solution to a higher-order linear differene equation and existene of bounded solutions

More information

A two storage inventory model with variable demand and time dependent deterioration rate and with partial backlogging

A two storage inventory model with variable demand and time dependent deterioration rate and with partial backlogging Malaya Journal of Matematik, Vol. S, No., 35-40, 08 https://doi.org/0.37/mjm0s0/07 A two storage inventory model with variable demand and time dependent deterioration rate and with partial baklogging Rihi

More information

CHAPTER P Preparation for Calculus

CHAPTER P Preparation for Calculus PART I CHAPTER P Preparation for Calulus Setion P. Graphs and Models...................... Setion P. Linear Models and Rates of Change............. 7 Setion P. Funtions and Their Graphs.................

More information

Geometry of Transformations of Random Variables

Geometry of Transformations of Random Variables Geometry of Transformations of Random Variables Univariate distributions We are interested in the problem of finding the distribution of Y = h(x) when the transformation h is one-to-one so that there is

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 Novel Process for the Study of Breakage Energy versus Particle Size

A Novel Process for the Study of Breakage Energy versus Particle Size Geomaterials, 2013, 3, 102-110 http://dx.doi.org/10.4236/gm.2013.33013 Published Online July 2013 (http://www.sirp.org/journal/gm) A Novel Proess for the Study of Breakage Energy versus Partile Size Elias

More information

Physics 486. Classical Newton s laws Motion of bodies described in terms of initial conditions by specifying x(t), v(t).

Physics 486. Classical Newton s laws Motion of bodies described in terms of initial conditions by specifying x(t), v(t). Physis 486 Tony M. Liss Leture 1 Why quantum mehanis? Quantum vs. lassial mehanis: Classial Newton s laws Motion of bodies desribed in terms of initial onditions by speifying x(t), v(t). Hugely suessful

More information

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM NETWORK SIMPLEX LGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM Cen Çalışan, Utah Valley University, 800 W. University Parway, Orem, UT 84058, 801-863-6487, en.alisan@uvu.edu BSTRCT The minimum

More information

A NORMALIZED EQUATION OF AXIALLY LOADED PILES IN ELASTO-PLASTIC SOIL

A NORMALIZED EQUATION OF AXIALLY LOADED PILES IN ELASTO-PLASTIC SOIL Journal of Geongineering, Vol. Yi-Chuan 4, No. 1, Chou pp. 1-7, and April Yun-Mei 009 Hsiung: A Normalized quation of Axially Loaded Piles in lasto-plasti Soil 1 A NORMALIZD QUATION OF AXIALLY LOADD PILS

More information