An Interpretation of the Black Energy in Universe by Using a Hydro-Dynamical Analogy with Newton Gravity

Size: px
Start display at page:

Download "An Interpretation of the Black Energy in Universe by Using a Hydro-Dynamical Analogy with Newton Gravity"

Transcription

1 An Interpretation of the Black nergy in Universe by Using a Hydro-Dynamical Analogy with Newton Gravity Corneli BRBNT*,1, Sorin BRBNT *Corresponding athor *,1 POLITHNICA University of Bcharest, Faclty of Aerospace ngineering, Department lie Carafoli Aerospace Science, Poliz Street 1-, postal code 011, sector 1, Bcharest, berbente@yahoo.com INCAS National Institte for Aerospace Research lie Carafoli, B-dl Ili Mani 0, Sector, Bcharest 011, Romania berbente.sorin@incas.ro DOI:.13111/ Received: 8 October 018/ Accepted: 14 November 018/ Pblished: December 018 Copyright 018. Pblished by INCAS. This is an open access article nder the CC BY-NC-ND license ( International Conference of Aerospace Sciences AROSPATIAL October 018, Bcharest, Romania, (held at INCAS, B-dl Ili Mani 0, sector ) Section 3 Astronatics and Astrophysics Abstract: There are arments proving that what we see now as normal energy (inclding the eqivalent mass-energy) represents only 5% of the total energy of the Universe [1]. The rest is invisible meaning that no widely accepted experimental proof exits to pt it in evidence. In addition, there is no accepted theory to explain the natre of this so-called black energy. This paper deals with an interpretation of the black energy also giving the possibility to follow its evoltion in time by sing an athor hydro-dynamical model of the Newton gravity and a model of the early Universe; a connection between a part of this energy and the black holes is as well proposed. Key Words: flid of HD-gravitons, variable gravity coefficient, emission, absorption 1. INTRODUCTION The spposition that the known matter and energy observed in or Universe does not represent all the existing ones is probably old enogh. However, in the last time qantitative vales for the possible existing percentages of black energy (8.3%) and black matter (.8%) were given [1]. A possible interpretation of sch big percentages is sggested by or hydro-dynamical analogy with gravity []. The main idea of this model is the analogy between the Newton gravity force and the sorces interaction in an incompressible flid. In this case the flid is formed of photon-like particles that we call HD-gravitons. Or HDgraviton is the weakest possible particle in Universe having the wave length eqal to the radis of the Universe. Ths it is very hard (if not impossible) to detect. Therefore, at BIG BANG (better said BIG FLASH as the sond does not propagate throgh vacm) the whole energy of the Universe is in the form of a single HD-graviton; that means that in fact what is now called black energy is the very energy of the created Universe and what one has rather to do is to explain the formation of the visible energy. To this aim we se the simple INCAS BULLTIN, Volme, Isse 4/ 018, pp (P) ISSN 0-801, () ISSN 4-458

2 Corneli BRBNT, Sorin BRBNT 14 physical- geometrical model of the early Universe given in [3]. In this model one attaches to any amont of energy a photon-like particle of the same energy whose wave length is sed to associate a radis of a sphere. Then by considering a simple geometrical model coming from the observation that the minimm nmber of eqal spheres that can enter in a sphere is eleven one attaches a strctring scheme where all the spheres are filled sccessively with 11 spheres. The nmber of the strctring steps shold be clearly integer. The qestion is whether following this process one can obtain spheres having the same radis and energy as their associated photon. This is possible as we shall prove frther. According to or hydro-dynamical analogy, if is an arbitrary amont of energy (other than HD-graviton) it can emit/absorb a rate of energy eqal to:, (1) g being the rate intensity ( g sec 1 ), which is positive for emission and negative for absorption. There is force of attraction for both emission and absorption, similar to the gravity force. By comparing the Newton and the sorce forces one obtains an expression for the intensity. The form given in Ref. [] is adapted to take into accont the dimintion of the HD-graviton intensity de to the Universe expansion and the variation of the niversal coefficient of gravity with the age of niverse. t g. DTRMINATION OF TH TOTAL NRGY OF TH UNIVRS. TRANSFORMATION OF HD-GRAVITONS IN SUBSTANC As mentioned above, according to or model of the early Universe [3], after the BIG BANG (BIG FLASH) the created primary spherical photon-like particle is sbmitted to a process of divisions in eleven eqal spheres (the minimm nmber of eqal spheres that can be inscribed in a given initial sphere, Fig. 1). By attaching to any amont of energy a photon of the same energy one obtains a vale for the radis of the 11 spheres eqal to the wave length of the associated photon. Then the radis of an inscribed sphere is increased 11 times, as the energy of the attached photon has been diminished 11 times. Fig. 1 Six of the eleven inscribed spheres (one confiration) INCAS BULLTIN, Volme, Isse 4/ 018

3 15 An Interpretation of the Black nergy in Universe by Using a Hydro-Dynamical Analogy with Newton Gravity From Fig. 1 one can see that at each division the radis of the initial sphere becomes three times the radis of an inscribed sphere. Ths, the radis of the srronding sphere increases 33 times at each division. Let be the radis of the Universe at BIG FLASH, eqal to the wave length of the photon R 0 associated to the total energy. One can write: Frther let s take: R hc V 0. () U 0 11 S, (3) ne0 ne0 being the energy of the netron at rest and S a nmber of divisions. One can write the following relations: gs R 33 R ; t R / c ; h c / R 33 3, (4) S S S S 0 S S V gs V S ne0 being the energy of a HD-graviton at time t ts. The wave length of the photon attached to a sphere (energy) for S= divisions (having the energy of a netron at rest) is m, whereas the radis of netron as ncleon is very close: r 15 ne 1. m (possible smaller in ncles). Therefore one can consider that, for S=, the spheres obtained by division have the energies and the radii eqal to a netron at rest and this represents a form of resonance permitting the transformation of energy in sbstance. Ths one obtains a netron from HDgravitons. Of corse, the spheres are at different speeds and the transformation itself will take a certain time from. For S= one obtains: 11 t.30 Jole; R.18 m; 0 1 U0 t l ys t l ys sec..43..; act One leaves time for the transformation of all HD-gravitons in sbstance and one introdces a time t HD representing the age of the Universe from where the hydro-dynamical analogy with Newton gravity law can be applied. From time 3. QUATION OF TRANSFORMATION NRGY-MATTR VIA GRAVITY t HD the hydro-dynamical analogy with Newton gravity starts to work. One will consider at t t HD that almost the whole Universe contains normal matter. Then the first transformation will be emission of HD-gravitons. The global eqation of transformation via emission/absorption of the average HD-graviton energy is. 3 (5) INCAS BULLTIN, Volme, Isse 4/ 018

4 Corneli BRBNT, Sorin BRBNT 1 d dt ( t )( ), () g The soltion of the differential eqation () depends on the intensity pt nder the form: N ref gu g tu thd t 5 ct V ref ( t ) g which can be 3 f 5 ( ). () where is the exponent of variation of the gravity coefficient We have sed the expression: f N with the age of Universe. ; 1 f t f N Nref t t ref. (8) To obtain the vale 1 we have sed information regarding the body systems with stable confiration on large time intervals. Sch is the system is the Sn- (arth-moon) known as being maintained for abot 4 billion years. The vale 1 is a very good approximation that will be extrapolated back in time p to t HD. The eqation () has the analytical soltion given bellow: 1 X 1 X At ( ) ref HD ref ln (1 ( ) ); 1X 1X ref tref t t (9-a) A t t 3 f t HD Nact act ( HD ) ; 5 cv X U0, (9-b) t ref being a reference (initial) time. The signs ( ) correspond to emission and absorption, respectively. One does not know exactly the critical vales of the ratio for the emission or the absorption to start. U 0 Anyhow the emission shold start when there is lack of HD-gravitons and the absorption, when there is excess of HD-gravitons. Therefore for the critical ratios at emission and absorption one writes: A t t 3 f t HD Nact act ( HD ) ; 5 cv X U0, () As regards t HD one takes two vales larger then t given in relation (5), namely: INCAS BULLTIN, Volme, Isse 4/ 018

5 1 An Interpretation of the Black nergy in Universe by Using a Hydro-Dynamical Analogy with Newton Gravity t ys.; t ys. (11) HD1 HD One interesting aim is to see whether the vales for the black energy and black matter given in Ref. [1] are possible by sing or model, staring from. The t HD1 and t HD calclations given in Table 1 indicate that several cycles emission-absorption are necessary to come in the neighborhood of a state from where one can arrive at the proposed vales at tact 1.38 ys. In Table 1the critical ratio / em was taken eqal for emission and absorption. This way, one cold execte an integer nmber of cycles emission- absorption: 9 for t thd1 ys. and 1 for t thd ys. The next transformations are emissions leading to a vale close enogh to nity in order to start absorptions at times capable to lead to the actal ratios / of the black energy (see Table 1). t HD, ys. act X 0.95 t absref X ref Table 1. voltions to the actal vales of the black energy X t 9em em, 8 8 ys Cycle nmber 1 X ref act t absref ( ys.) Remark. As one can see from the Table 1, the evoltion in cycles emission-absorption are taking place only in the early age of the Universe, representing at most 1% of the actal age, The transformation becomes more and more slow: only one transformation (absorption: there are reasons to consider that the Universe is now in absorption) takes place to arrive at the actal age. 4. CONSIDRATIONS RGARDING TH BLACK MATTR. FUTUR VOLUTION According to Ref. [1] the black matter wold represent now.8% of the total energy of the Universe ( ). We consider that a part of this black matter cold be associated to black holes. ven in the vicinity of the critical vale of the ratio mass/ radis ((M/R) cr =.4 Kg/m, see [5]) for their formation, the black holes are srronded by a high density flid of HD-gravitons absorbed at their frontier. This cold have been considered black matter being in fact black energy. The high density form of energy cold be also connected to what is considered particles creation by black holes, in Ref. [4]. In conclsion the black energy percentage is in or opinion larger than 8.3%. In order to see the ftre evoltion of the black energy as well as the intensity of HDgraviton flx certain data are given in Table. INCAS BULLTIN, Volme, Isse 4/ 018

6 Corneli BRBNT, Sorin BRBNT 18 t HD, ys. Table. Absorption of HD-gravitons after ref - gref tact gfin ys. fin 5 5 From Table one can see that the rate of absorption increases with increasing of the intensity g proportionally with time the same dimintion of the total energy of HD-gravitons, t HD t HD t fin, ys becase of the. This shorts the time interval for. One also can see that small redctions of the black energy from now on reqires hndred millions or even billions of years, the transformation being more and more slow. As regards the intensity of the flx of HD-gravitons at the srface of a black hole, one can estimate for a black hole of mass M and radis R the vale: Mc c g g V g M V ( Watt / m ) R R R CR R R R, (1) where the critical (minimm) vale of ratio ( M / R) for the black hole formation was considered. The ratio (1) can be compared with the thermal energy flx at or Sn srface which is.3 Watt / m. For R RSUN 8m one obtains at least twelve orders of magnitde! 5. CONCLUSIONS The black energy in Universe is interpreted as the flid of HD-gravitons which is emitted or absorbed by bodies and particles (other then HD-gravitons). It is essential for the creation of gravity in Universe. A HD-graviton is a photon-like particle having a wave length eqal to the radis of Universe ths directly non-detectable. In fact, the existence of the flid of HD-gravitons is proved by the gravity itself. As regards the black matter a possible explanation of the percentage given in [1] is via the black holes even at the limit vale of the ratio mass/radis M / R for their formation CR Ths the mass of sch black holes cold be over - estimated de to the high intensity flid of HD-gravitons absorbed at their frontier. Therefore the main part of what is invisible comes to black energy. A balance eqation for the behavior of the black energy is given. Calclations proving the possibility of its existence even in larger percentages than reported are also given. INCAS BULLTIN, Volme, Isse 4/ 018

7 19 An Interpretation of the Black nergy in Universe by Using a Hydro-Dynamical Analogy with Newton Gravity RFRNCS [1] * * * [] C. Berbente, A Hydro-Dynamical Model for Gravity, INCAS Blletin, (online) ISSN 4 458, (print) ISSN 0 801, ISSN L 0 801, vol. 8, Isse 1, DOI:.13111/ , p.39-4, Jan.- March. 01. [3] C. Berbente, A Physical - Geometrical Model of an arly Universe, INCAS Blletin, (online) ISSN 4 458, (print) ISSN 0 801, ISSN L 0 801, vol., Isse 4, DOI:.13111/ , p. 3-1, Bcharest, Romania, 014. [4] S. W. Hawking, Particle Creation by Black Hole, Commnications in Mathem. Physics, 43, (3), p.199-0, 195. [5] C. Berbente, S. Berbente, Possible Simple Strctres of the Universe to Inclde General Relativity ffects, INCAS Blletin, (online) ISSN 4 458, (print) ISSN 0 801, ISSN L 0 801, vol. 9, Isse 4, p.11-0, Oct.- December, 01. INCAS BULLTIN, Volme, Isse 4/ 018

Possible holographic universe, graviton rest mass, mass gap and dark energy

Possible holographic universe, graviton rest mass, mass gap and dark energy JJJPL report 0423-2 (2015); vixra:1508.0292 (2015). Possible holographic niverse, graviton rest mass, mass gap and dark energy Jae-Kwang Hwang JJJ Physics Laboratory, 1077 Beech Tree Lane, Brentwood, TN

More information

Copyright Canadian Institute of Steel Construction

Copyright Canadian Institute of Steel Construction Copyright 017 by Canadian Institte of Steel Constrction All rights reserved. This book or any part thereof mst not be reprodced in any form withot the written permission of the pblisher. Third Edition

More information

5. The Bernoulli Equation

5. The Bernoulli Equation 5. The Bernolli Eqation [This material relates predominantly to modles ELP034, ELP035] 5. Work and Energy 5. Bernolli s Eqation 5.3 An example of the se of Bernolli s eqation 5.4 Pressre head, velocity

More information

1. INTRODUCTION. A solution for the dark matter mystery based on Euclidean relativity. Frédéric LASSIAILLE 2009 Page 1 14/05/2010. Frédéric LASSIAILLE

1. INTRODUCTION. A solution for the dark matter mystery based on Euclidean relativity. Frédéric LASSIAILLE 2009 Page 1 14/05/2010. Frédéric LASSIAILLE Frédéric LASSIAILLE 2009 Page 1 14/05/2010 Frédéric LASSIAILLE email: lmimi2003@hotmail.com http://lmi.chez-alice.fr/anglais A soltion for the dark matter mystery based on Eclidean relativity The stdy

More information

L = 2 λ 2 = λ (1) In other words, the wavelength of the wave in question equals to the string length,

L = 2 λ 2 = λ (1) In other words, the wavelength of the wave in question equals to the string length, PHY 309 L. Soltions for Problem set # 6. Textbook problem Q.20 at the end of chapter 5: For any standing wave on a string, the distance between neighboring nodes is λ/2, one half of the wavelength. The

More information

4 Exact laminar boundary layer solutions

4 Exact laminar boundary layer solutions 4 Eact laminar bondary layer soltions 4.1 Bondary layer on a flat plate (Blasis 1908 In Sec. 3, we derived the bondary layer eqations for 2D incompressible flow of constant viscosity past a weakly crved

More information

Two questions from the exam

Two questions from the exam Two qestions from the exam 3. When the sn is located near one of the horizons, an observer looking at the sky directly overhead will view partially polarized light. This effect is de to which of the following

More information

Replacement of Einstein s Relativity Theory with a New One: Why the Second Postulate is Superfluous?

Replacement of Einstein s Relativity Theory with a New One: Why the Second Postulate is Superfluous? International Jornal of Physics, 16, Vol. 4, No. 5, 14-145 Available online at http://pbs.sciepb.com/ijp/4/5/5 Science and Edcation Pblishing DOI:1.1691/ijp-4-5-5 Replacement of Einstein s Relativity Theory

More information

UNIT V BOUNDARY LAYER INTRODUCTION

UNIT V BOUNDARY LAYER INTRODUCTION UNIT V BOUNDARY LAYER INTRODUCTION The variation of velocity from zero to free-stream velocity in the direction normal to the bondary takes place in a narrow region in the vicinity of solid bondary. This

More information

Chem 4501 Introduction to Thermodynamics, 3 Credits Kinetics, and Statistical Mechanics. Fall Semester Homework Problem Set Number 10 Solutions

Chem 4501 Introduction to Thermodynamics, 3 Credits Kinetics, and Statistical Mechanics. Fall Semester Homework Problem Set Number 10 Solutions Chem 4501 Introdction to Thermodynamics, 3 Credits Kinetics, and Statistical Mechanics Fall Semester 2017 Homework Problem Set Nmber 10 Soltions 1. McQarrie and Simon, 10-4. Paraphrase: Apply Eler s theorem

More information

Second-Order Wave Equation

Second-Order Wave Equation Second-Order Wave Eqation A. Salih Department of Aerospace Engineering Indian Institte of Space Science and Technology, Thirvananthapram 3 December 016 1 Introdction The classical wave eqation is a second-order

More information

Numerical Study on Bouncing and Separation Collision Between Two Droplets Considering the Collision-Induced Breakup

Numerical Study on Bouncing and Separation Collision Between Two Droplets Considering the Collision-Induced Breakup Jornal of Mechanical Science and Technology (007) 585~59 Jornal of Mechanical Science and Technology Nmerical Stdy on Boncing and Separation Collision Between Two Droplets Considering the Collision-Indced

More information

Designing of Virtual Experiments for the Physics Class

Designing of Virtual Experiments for the Physics Class Designing of Virtal Experiments for the Physics Class Marin Oprea, Cristina Miron Faclty of Physics, University of Bcharest, Bcharest-Magrele, Romania E-mail: opreamarin2007@yahoo.com Abstract Physics

More information

Study of the diffusion operator by the SPH method

Study of the diffusion operator by the SPH method IOSR Jornal of Mechanical and Civil Engineering (IOSR-JMCE) e-issn: 2278-684,p-ISSN: 2320-334X, Volme, Isse 5 Ver. I (Sep- Oct. 204), PP 96-0 Stdy of the diffsion operator by the SPH method Abdelabbar.Nait

More information

Report and Opinion 2017;9(4s) 1.Mathematical Theory of Space-Time. Jiang Chunxuan

Report and Opinion 2017;9(4s)   1.Mathematical Theory of Space-Time. Jiang Chunxuan athematical Theory Of Space-Time Jiang Chnxan Institte for asic esearch, Palm Harbor, FL3468-1577, USA And: P O ox 394, eijing 100854, P China jiangchnxan@sohcom, cxjiang@mailbcfnetcn, jcxan@sinacom, Jiangchnxan@vipsohcom,

More information

Two-media boundary layer on a flat plate

Two-media boundary layer on a flat plate Two-media bondary layer on a flat plate Nikolay Ilyich Klyev, Asgat Gatyatovich Gimadiev, Yriy Alekseevich Krykov Samara State University, Samara,, Rssia Samara State Aerospace University named after academician

More information

Reduction of over-determined systems of differential equations

Reduction of over-determined systems of differential equations Redction of oer-determined systems of differential eqations Maim Zaytse 1) 1, ) and Vyachesla Akkerman 1) Nclear Safety Institte, Rssian Academy of Sciences, Moscow, 115191 Rssia ) Department of Mechanical

More information

EXPT. 5 DETERMINATION OF pk a OF AN INDICATOR USING SPECTROPHOTOMETRY

EXPT. 5 DETERMINATION OF pk a OF AN INDICATOR USING SPECTROPHOTOMETRY EXPT. 5 DETERMITIO OF pk a OF IDICTOR USIG SPECTROPHOTOMETRY Strctre 5.1 Introdction Objectives 5.2 Principle 5.3 Spectrophotometric Determination of pka Vale of Indicator 5.4 Reqirements 5.5 Soltions

More information

Classify by number of ports and examine the possible structures that result. Using only one-port elements, no more than two elements can be assembled.

Classify by number of ports and examine the possible structures that result. Using only one-port elements, no more than two elements can be assembled. Jnction elements in network models. Classify by nmber of ports and examine the possible strctres that reslt. Using only one-port elements, no more than two elements can be assembled. Combining two two-ports

More information

1 Introduction. r + _

1 Introduction. r + _ A method and an algorithm for obtaining the Stable Oscillator Regimes Parameters of the Nonlinear Sstems, with two time constants and Rela with Dela and Hsteresis NUŢU VASILE, MOLDOVEANU CRISTIAN-EMIL,

More information

PhysicsAndMathsTutor.com

PhysicsAndMathsTutor.com . Two smooth niform spheres S and T have eqal radii. The mass of S is 0. kg and the mass of T is 0.6 kg. The spheres are moving on a smooth horizontal plane and collide obliqely. Immediately before the

More information

Study on the impulsive pressure of tank oscillating by force towards multiple degrees of freedom

Study on the impulsive pressure of tank oscillating by force towards multiple degrees of freedom EPJ Web of Conferences 80, 0034 (08) EFM 07 Stdy on the implsive pressre of tank oscillating by force towards mltiple degrees of freedom Shigeyki Hibi,* The ational Defense Academy, Department of Mechanical

More information

BLOOM S TAXONOMY. Following Bloom s Taxonomy to Assess Students

BLOOM S TAXONOMY. Following Bloom s Taxonomy to Assess Students BLOOM S TAXONOMY Topic Following Bloom s Taonomy to Assess Stdents Smmary A handot for stdents to eplain Bloom s taonomy that is sed for item writing and test constrction to test stdents to see if they

More information

Radiation Effects on Heat and Mass Transfer over an Exponentially Accelerated Infinite Vertical Plate with Chemical Reaction

Radiation Effects on Heat and Mass Transfer over an Exponentially Accelerated Infinite Vertical Plate with Chemical Reaction Radiation Effects on Heat and Mass Transfer over an Exponentially Accelerated Infinite Vertical Plate with Chemical Reaction A. Ahmed, M. N.Sarki, M. Ahmad Abstract In this paper the stdy of nsteady flow

More information

Solutions to Math 152 Review Problems for Exam 1

Solutions to Math 152 Review Problems for Exam 1 Soltions to Math 5 Review Problems for Eam () If A() is the area of the rectangle formed when the solid is sliced at perpendiclar to the -ais, then A() = ( ), becase the height of the rectangle is and

More information

Computations of the Shock Waves at Hypersonic Velocities Taken into Account the Chemical Reactions that Appear in the Air at High Temperatures

Computations of the Shock Waves at Hypersonic Velocities Taken into Account the Chemical Reactions that Appear in the Air at High Temperatures Comtations of the Shock Waves at Hyersonic Velocities aken into Accont the Chemical Reactions that Aear in the Air at High emeratres Mihai Leonida NICLESC*,, Maris Gabriel COJOCAR Mihai Victor PRICOP,

More information

Cosmic rays. l Some come from the sun (relatively low energy) and some from catastrophic events elsewhere in the galaxy/universe

Cosmic rays. l Some come from the sun (relatively low energy) and some from catastrophic events elsewhere in the galaxy/universe Special relativity The laws of physics are the same in all coordinate systems either at rest or moving at constant speed with respect to one another The speed of light in a vacm has the same vale regardless

More information

Lewis number and curvature effects on sound generation by premixed flame annihilation

Lewis number and curvature effects on sound generation by premixed flame annihilation Center for Trblence Research Proceedings of the Smmer Program 2 28 Lewis nmber and crvatre effects on sond generation by premixed flame annihilation By M. Talei, M. J. Brear AND E. R. Hawkes A nmerical

More information

VIBRATION MEASUREMENT UNCERTAINTY AND RELIABILITY DIAGNOSTICS RESULTS IN ROTATING SYSTEMS

VIBRATION MEASUREMENT UNCERTAINTY AND RELIABILITY DIAGNOSTICS RESULTS IN ROTATING SYSTEMS VIBRATIO MEASUREMET UCERTAITY AD RELIABILITY DIAGOSTICS RESULTS I ROTATIG SYSTEMS. Introdction M. Eidkevicite, V. Volkovas anas University of Technology, Lithania The rotating machinery technical state

More information

STEP Support Programme. STEP III Hyperbolic Functions: Solutions

STEP Support Programme. STEP III Hyperbolic Functions: Solutions STEP Spport Programme STEP III Hyperbolic Fnctions: Soltions Start by sing the sbstittion t cosh x. This gives: sinh x cosh a cosh x cosh a sinh x t sinh x dt t dt t + ln t ln t + ln cosh a ln ln cosh

More information

The Influence of Aerodynamic Characteristics of the Elements of the Flow Range of the Radial Two-row Microturbine on its Dynamic Characteristics

The Influence of Aerodynamic Characteristics of the Elements of the Flow Range of the Radial Two-row Microturbine on its Dynamic Characteristics International Jornal of Applied Engineering Research ISSN 097-56 Volme 11, Nmber (016) pp. 11501-11509 The Inflence of Aerodynamic Characteristics of the Elements of the Flow Range of the Radial Two-row

More information

Effects of modifications on the hydraulics of Denil fishways

Effects of modifications on the hydraulics of Denil fishways BOREAL ENVIRONMENT RESEARCH 5: 67 79 ISSN 1239-6095 Helsinki 28 March 2000 2000 Effects of modifications on the hydralics of Denil fishways Riitta Kamla 1) and Jan Bärthel 2) 1) Water Resorces and Environmental

More information

Applying Laminar and Turbulent Flow and measuring Velocity Profile Using MATLAB

Applying Laminar and Turbulent Flow and measuring Velocity Profile Using MATLAB IOS Jornal of Mathematics (IOS-JM) e-issn: 78-578, p-issn: 319-765X. Volme 13, Isse 6 Ver. II (Nov. - Dec. 17), PP 5-59 www.iosrjornals.org Applying Laminar and Trblent Flow and measring Velocity Profile

More information

A New Approach to Direct Sequential Simulation that Accounts for the Proportional Effect: Direct Lognormal Simulation

A New Approach to Direct Sequential Simulation that Accounts for the Proportional Effect: Direct Lognormal Simulation A ew Approach to Direct eqential imlation that Acconts for the Proportional ffect: Direct ognormal imlation John Manchk, Oy eangthong and Clayton Detsch Department of Civil & nvironmental ngineering University

More information

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA. PRINCIPLES AND APPLICATIONS of FLUID MECHANICS UNIT 13 NQF LEVEL 3 OUTCOME 3 - HYDRODYNAMICS

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA. PRINCIPLES AND APPLICATIONS of FLUID MECHANICS UNIT 13 NQF LEVEL 3 OUTCOME 3 - HYDRODYNAMICS EDEXCEL NATIONAL CERTIFICATE/DIPLOMA PRINCIPLES AND APPLICATIONS of FLUID MECHANICS UNIT 3 NQF LEVEL 3 OUTCOME 3 - HYDRODYNAMICS TUTORIAL - PIPE FLOW CONTENT Be able to determine the parameters of pipeline

More information

MODELLING OF TURBULENT ENERGY FLUX IN CANONICAL SHOCK-TURBULENCE INTERACTION

MODELLING OF TURBULENT ENERGY FLUX IN CANONICAL SHOCK-TURBULENCE INTERACTION MODELLING OF TURBULENT ENERGY FLUX IN CANONICAL SHOCK-TURBULENCE INTERACTION Rssell Qadros, Krishnend Sinha Department of Aerospace Engineering Indian Institte of Technology Bombay Mmbai, India 476 Johan

More information

Available online at ScienceDirect. Procedia Engineering 150 (2016 )

Available online at   ScienceDirect. Procedia Engineering 150 (2016 ) Available online at www.sciencedirect.com ScienceDirect Procedia Engineering 150 (016 ) 635 640 International Conference on Indstrial Engineering, ICIE 016 Research of Dynamics of the Rotor with Three-film

More information

A Decomposition Method for Volume Flux. and Average Velocity of Thin Film Flow. of a Third Grade Fluid Down an Inclined Plane

A Decomposition Method for Volume Flux. and Average Velocity of Thin Film Flow. of a Third Grade Fluid Down an Inclined Plane Adv. Theor. Appl. Mech., Vol. 1, 8, no. 1, 9 A Decomposition Method for Volme Flx and Average Velocit of Thin Film Flow of a Third Grade Flid Down an Inclined Plane A. Sadighi, D.D. Ganji,. Sabzehmeidani

More information

An Investigation into Estimating Type B Degrees of Freedom

An Investigation into Estimating Type B Degrees of Freedom An Investigation into Estimating Type B Degrees of H. Castrp President, Integrated Sciences Grop Jne, 00 Backgrond The degrees of freedom associated with an ncertainty estimate qantifies the amont of information

More information

Illustrations of a Modified Standard Model: Part 1-The Solar Proton- Proton Cycle

Illustrations of a Modified Standard Model: Part 1-The Solar Proton- Proton Cycle Illstrations of a Modified : Part 1-The Solar Proton- Proton Cycle by Roger N. Weller, (proton3@gmail.com), Febrary 23, 2014 Abstract A proposed modification of the, when applied to the Solar Proton-Proton

More information

Active Flux Schemes for Advection Diffusion

Active Flux Schemes for Advection Diffusion AIAA Aviation - Jne, Dallas, TX nd AIAA Comptational Flid Dynamics Conference AIAA - Active Fl Schemes for Advection Diffsion Hiroaki Nishikawa National Institte of Aerospace, Hampton, VA 3, USA Downloaded

More information

Math 144 Activity #10 Applications of Vectors

Math 144 Activity #10 Applications of Vectors 144 p 1 Math 144 Actiity #10 Applications of Vectors In the last actiity, yo were introdced to ectors. In this actiity yo will look at some of the applications of ectors. Let the position ector = a, b

More information

Effects of Soil Spatial Variability on Bearing Capacity of Shallow Foundations

Effects of Soil Spatial Variability on Bearing Capacity of Shallow Foundations Geotechnical Safety and Risk V T. Schweckendiek et al. (Eds.) 2015 The athors and IOS Press. This article is pblished online with Open Access by IOS Press and distribted nder the terms of the Creative

More information

FEA Solution Procedure

FEA Solution Procedure EA Soltion Procedre (demonstrated with a -D bar element problem) EA Procedre for Static Analysis. Prepare the E model a. discretize (mesh) the strctre b. prescribe loads c. prescribe spports. Perform calclations

More information

Research Article Permanence of a Discrete Predator-Prey Systems with Beddington-DeAngelis Functional Response and Feedback Controls

Research Article Permanence of a Discrete Predator-Prey Systems with Beddington-DeAngelis Functional Response and Feedback Controls Hindawi Pblishing Corporation Discrete Dynamics in Natre and Society Volme 2008 Article ID 149267 8 pages doi:101155/2008/149267 Research Article Permanence of a Discrete Predator-Prey Systems with Beddington-DeAngelis

More information

entropy ISSN by MDPI

entropy ISSN by MDPI Entropy, 007, 9, 113-117 Letter to the Editor entropy ISSN 1099-4300 007 by MDPI www.mdpi.org/entropy Entropy of Relativistic Mono-Atomic Gas and Temperatre Relativistic Transformation in Thermodynamics

More information

Chapter 3 MATHEMATICAL MODELING OF DYNAMIC SYSTEMS

Chapter 3 MATHEMATICAL MODELING OF DYNAMIC SYSTEMS Chapter 3 MATHEMATICAL MODELING OF DYNAMIC SYSTEMS 3. System Modeling Mathematical Modeling In designing control systems we mst be able to model engineered system dynamics. The model of a dynamic system

More information

EXCITATION RATE COEFFICIENTS OF MOLYBDENUM ATOM AND IONS IN ASTROPHYSICAL PLASMA AS A FUNCTION OF ELECTRON TEMPERATURE

EXCITATION RATE COEFFICIENTS OF MOLYBDENUM ATOM AND IONS IN ASTROPHYSICAL PLASMA AS A FUNCTION OF ELECTRON TEMPERATURE EXCITATION RATE COEFFICIENTS OF MOLYBDENUM ATOM AND IONS IN ASTROPHYSICAL PLASMA AS A FUNCTION OF ELECTRON TEMPERATURE A.N. Jadhav Department of Electronics, Yeshwant Mahavidyalaya, Ned. Affiliated to

More information

Model Explaining the Gravitational Force

Model Explaining the Gravitational Force Model Explaining the Gravitational Force Clade Mercier eng., Agst nd, 015 Rev. October 17 th, 015 clade.mercier@gctda.com The niversal gravitation eqation of Newton is widely sed in the calclations in

More information

Formal Methods for Deriving Element Equations

Formal Methods for Deriving Element Equations Formal Methods for Deriving Element Eqations And the importance of Shape Fnctions Formal Methods In previos lectres we obtained a bar element s stiffness eqations sing the Direct Method to obtain eact

More information

Queueing analysis of service deferrals for load management in power systems

Queueing analysis of service deferrals for load management in power systems Qeeing analysis of service deferrals for load management in power systems Andrés Ferragt and Fernando Paganini Universidad ORT Urgay Abstract With the advent of renewable sorces and Smart- Grid deployments,

More information

Introdction Finite elds play an increasingly important role in modern digital commnication systems. Typical areas of applications are cryptographic sc

Introdction Finite elds play an increasingly important role in modern digital commnication systems. Typical areas of applications are cryptographic sc A New Architectre for a Parallel Finite Field Mltiplier with Low Complexity Based on Composite Fields Christof Paar y IEEE Transactions on Compters, Jly 996, vol 45, no 7, pp 856-86 Abstract In this paper

More information

University of California, Berkeley Physics H7C Fall 1999 (Strovink) SOLUTION TO FINAL EXAMINATION

University of California, Berkeley Physics H7C Fall 1999 (Strovink) SOLUTION TO FINAL EXAMINATION University of California Berkeley Physics H7C Fall 999 (Strovink SOUTION TO FINA EXAMINATION Directions. Do all six problems (weights are indicated. This is a closed-book closed-note exam except for three

More information

PROBLEMS

PROBLEMS PROBLEMS------------------------------------------------ - 7- Thermodynamic Variables and the Eqation of State 1. Compter (a) the nmber of moles and (b) the nmber of molecles in 1.00 cm of an ideal gas

More information

UNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL

UNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL 8th International DAAAM Baltic Conference "INDUSTRIAL ENGINEERING - 19-1 April 01, Tallinn, Estonia UNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL Põdra, P. & Laaneots, R. Abstract: Strength analysis is a

More information

Efficiency Increase and Input Power Decrease of Converted Prototype Pump Performance

Efficiency Increase and Input Power Decrease of Converted Prototype Pump Performance International Jornal of Flid Machinery and Systems DOI: http://dx.doi.org/10.593/ijfms.016.9.3.05 Vol. 9, No. 3, Jly-September 016 ISSN (Online): 188-9554 Original Paper Efficiency Increase and Inpt Power

More information

Lecture Notes: Finite Element Analysis, J.E. Akin, Rice University

Lecture Notes: Finite Element Analysis, J.E. Akin, Rice University 9. TRUSS ANALYSIS... 1 9.1 PLANAR TRUSS... 1 9. SPACE TRUSS... 11 9.3 SUMMARY... 1 9.4 EXERCISES... 15 9. Trss analysis 9.1 Planar trss: The differential eqation for the eqilibrim of an elastic bar (above)

More information

Elements of Coordinate System Transformations

Elements of Coordinate System Transformations B Elements of Coordinate System Transformations Coordinate system transformation is a powerfl tool for solving many geometrical and kinematic problems that pertain to the design of gear ctting tools and

More information

Particles and fields. Today: Review Particle Physics. Question. Quantum Electrodynamics: QED. Electrons and photons

Particles and fields. Today: Review Particle Physics. Question. Quantum Electrodynamics: QED. Electrons and photons Exam 4: Fri. May 10, in-class 20 qestions, covers fission, fsion, particle physics No final exam. Essays retrne Friay Toay: Review Particle Physics Particles an fiels: a new pictre Qarks an leptons The

More information

Design and Data Acquisition for Thermal Conductivity Matric Suction Sensors

Design and Data Acquisition for Thermal Conductivity Matric Suction Sensors 68 TRANSPORTATION RSARCH RCORD 1432 Design and Data Acqisition for Thermal Condctivity Matric Sction Sensors J. K.-M. GAN, D. G. FRDLUND, A. XING, AND W.-X. LI The principles behind sing the thermal condctivity

More information

Regression Analysis of Octal Rings as Mechanical Force Transducers

Regression Analysis of Octal Rings as Mechanical Force Transducers Regression Analysis of Octal Rings as Mechanical Force Transdcers KHALED A. ABUHASEL* & ESSAM SOLIMAN** *Department of Mechanical Engineering College of Engineering, University of Bisha, Bisha, Kingdom

More information

FEA Solution Procedure

FEA Solution Procedure EA Soltion Procedre (demonstrated with a -D bar element problem) MAE 5 - inite Element Analysis Several slides from this set are adapted from B.S. Altan, Michigan Technological University EA Procedre for

More information

PhysicsAndMathsTutor.com

PhysicsAndMathsTutor.com C Integration - By sbstittion PhysicsAndMathsTtor.com. Using the sbstittion cos +, or otherwise, show that e cos + sin d e(e ) (Total marks). (a) Using the sbstittion cos, or otherwise, find the eact vale

More information

EVALUATION OF GROUND STRAIN FROM IN SITU DYNAMIC RESPONSE

EVALUATION OF GROUND STRAIN FROM IN SITU DYNAMIC RESPONSE 13 th World Conference on Earthqake Engineering Vancover, B.C., Canada Agst 1-6, 2004 Paper No. 3099 EVALUATION OF GROUND STRAIN FROM IN SITU DYNAMIC RESPONSE Ellen M. RATHJE 1, Wen-Jong CHANG 2, Kenneth

More information

OPTIMUM EXPRESSION FOR COMPUTATION OF THE GRAVITY FIELD OF A POLYHEDRAL BODY WITH LINEARLY INCREASING DENSITY 1

OPTIMUM EXPRESSION FOR COMPUTATION OF THE GRAVITY FIELD OF A POLYHEDRAL BODY WITH LINEARLY INCREASING DENSITY 1 OPTIMUM EXPRESSION FOR COMPUTATION OF THE GRAVITY FIEL OF A POLYHERAL BOY WITH LINEARLY INCREASING ENSITY 1 V. POHÁNKA2 Abstract The formla for the comptation of the gravity field of a polyhedral body

More information

Shape Phase Transition of Polyampholytes in. Two Dimensions. M. R. Ejtehadi and S. Rouhani. Department of Physics, Sharif University of Technology,

Shape Phase Transition of Polyampholytes in. Two Dimensions. M. R. Ejtehadi and S. Rouhani. Department of Physics, Sharif University of Technology, IPM # 1996 Shape Phase Transition of Polyampholytes in Two Dimensions M. R. Ejtehadi and S. Rohani Department of Physics, Sharif University of Technology, Tehran P. O. Box: 11365-5531, Iran. and Institte

More information

Math 116 First Midterm October 14, 2009

Math 116 First Midterm October 14, 2009 Math 116 First Midterm October 14, 9 Name: EXAM SOLUTIONS Instrctor: Section: 1. Do not open this exam ntil yo are told to do so.. This exam has 1 pages inclding this cover. There are 9 problems. Note

More information

APPLICATION OF MICROTREMOR MEASUREMENTS TO EARTHQUAKE ENGINEERING

APPLICATION OF MICROTREMOR MEASUREMENTS TO EARTHQUAKE ENGINEERING 170 APPLICATION OF MICROTREMOR MEASUREMENTS TO EARTHQUAKE ENGINEERING I. M. Parton* and P. W. Taylor* INTRODUCTION Two previos papers pblished in this Blletin (Refs 1, 2) described the methods developed

More information

FEA Solution Procedure

FEA Solution Procedure EA Soltion rocedre (demonstrated with a -D bar element problem) MAE - inite Element Analysis Many slides from this set are originally from B.S. Altan, Michigan Technological U. EA rocedre for Static Analysis.

More information

Partial Differential Equations with Applications

Partial Differential Equations with Applications Universit of Leeds MATH 33 Partial Differential Eqations with Applications Eamples to spplement Chapter on First Order PDEs Eample (Simple linear eqation, k + = 0, (, 0) = ϕ(), k a constant.) The characteristic

More information

Momentum Equation. Necessary because body is not made up of a fixed assembly of particles Its volume is the same however Imaginary

Momentum Equation. Necessary because body is not made up of a fixed assembly of particles Its volume is the same however Imaginary Momentm Eqation Interest in the momentm eqation: Qantification of proplsion rates esign strctres for power generation esign of pipeline systems to withstand forces at bends and other places where the flow

More information

Ted Pedersen. Southern Methodist University. large sample assumptions implicit in traditional goodness

Ted Pedersen. Southern Methodist University. large sample assumptions implicit in traditional goodness Appears in the Proceedings of the Soth-Central SAS Users Grop Conference (SCSUG-96), Astin, TX, Oct 27-29, 1996 Fishing for Exactness Ted Pedersen Department of Compter Science & Engineering Sothern Methodist

More information

STATIC, STAGNATION, AND DYNAMIC PRESSURES

STATIC, STAGNATION, AND DYNAMIC PRESSURES STATIC, STAGNATION, AND DYNAMIC PRESSURES Bernolli eqation is g constant In this eqation is called static ressre, becase it is the ressre that wold be measred by an instrment that is static with resect

More information

Step-Size Bounds Analysis of the Generalized Multidelay Adaptive Filter

Step-Size Bounds Analysis of the Generalized Multidelay Adaptive Filter WCE 007 Jly - 4 007 London UK Step-Size onds Analysis of the Generalized Mltidelay Adaptive Filter Jnghsi Lee and Hs Chang Hang Abstract In this paper we analyze the bonds of the fixed common step-size

More information

The Open Civil Engineering Journal

The Open Civil Engineering Journal Send Orders for Reprints to reprints@benthamscience.ae 564 The Open Ciil Engineering Jornal, 16, 1, 564-57 The Open Ciil Engineering Jornal Content list aailable at: www.benthamopen.com/tociej/ DOI: 1.174/187414951611564

More information

Higher Maths A1.3 Recurrence Relations - Revision

Higher Maths A1.3 Recurrence Relations - Revision Higher Maths A Recrrence Relations - Revision This revision pack covers the skills at Unit Assessment exam level or Recrrence Relations so yo can evalate yor learning o this otcome It is important that

More information

Chapter 9 Flow over Immersed Bodies

Chapter 9 Flow over Immersed Bodies 57:00 Mechanics o Flids and Transport Processes Chapter 9 Proessor Fred Stern Fall 01 1 Chapter 9 Flow over Immersed Bodies Flid lows are broadly categorized: 1. Internal lows sch as dcts/pipes, trbomachinery,

More information

Sareban: Evaluation of Three Common Algorithms for Structure Active Control

Sareban: Evaluation of Three Common Algorithms for Structure Active Control Engineering, Technology & Applied Science Research Vol. 7, No. 3, 2017, 1638-1646 1638 Evalation of Three Common Algorithms for Strctre Active Control Mohammad Sareban Department of Civil Engineering Shahrood

More information

THE REDUCTION IN FINESTRUCTURE CONTAMINATION OF INTERNAL WAVE ESTIMATES FROM A TOWED THERMISTOR CHAIN

THE REDUCTION IN FINESTRUCTURE CONTAMINATION OF INTERNAL WAVE ESTIMATES FROM A TOWED THERMISTOR CHAIN DANIEL C. DUBBEL THE REDUCTION IN FINESTRUCTURE CONTAMINATION OF INTERNAL WAVE ESTIMATES FROM A TOWED THERMISTOR CHAIN Estimates of internal wave displacements based on towed thermistor array data have

More information

DEFINITION OF A NEW UO 2 F 2 DENSITY LAW FOR LOW- MODERATED SOLUTIONS (H/U < 20) AND CONSEQUENCES ON CRITICALITY SAFETY

DEFINITION OF A NEW UO 2 F 2 DENSITY LAW FOR LOW- MODERATED SOLUTIONS (H/U < 20) AND CONSEQUENCES ON CRITICALITY SAFETY DEFINITION OF A NEW UO 2 F 2 DENSITY LAW FOR LOW- MODERATED SOLUTIONS ( < 20) AND CONSEQUENCES ON CRITICALITY SAFETY N. Leclaire, S. Evo, I.R.S.N., France Introdction In criticality stdies, the blk density

More information

Konyalioglu, Serpil. Konyalioglu, A.Cihan. Ipek, A.Sabri. Isik, Ahmet

Konyalioglu, Serpil. Konyalioglu, A.Cihan. Ipek, A.Sabri. Isik, Ahmet The Role of Visalization Approach on Stdent s Conceptal Learning Konyaliogl, Serpil Department of Secondary Science and Mathematics Edcation, K.K. Edcation Faclty, Atatürk University, 25240- Erzrm-Trkey;

More information

called the potential flow, and function φ is called the velocity potential.

called the potential flow, and function φ is called the velocity potential. J. Szantr Lectre No. 3 Potential flows 1 If the flid flow is irrotational, i.e. everwhere or almost everwhere in the field of flow there is rot 0 it means that there eists a scalar fnction ϕ,, z), sch

More information

FACULTY WORKING PAPER NO. 1081

FACULTY WORKING PAPER NO. 1081 35 51 COPY 2 FACULTY WORKING PAPER NO. 1081 Diagnostic Inference in Performance Evalation: Effects of Case and Event Covariation and Similarity Clifton Brown College of Commerce and Bsiness Administration

More information

Uncertainty Evaluation of Toluene Determination in Room Air by Thermal Desorption Gas Chromatography

Uncertainty Evaluation of Toluene Determination in Room Air by Thermal Desorption Gas Chromatography International Conference on Civil, Transportation and Environment (ICCTE 06) ncertainty Evalation of Tolene Determination in Room Air by Thermal Desorption Gas Chromatography Xiaoyan Wen, a,yanhi Gao,

More information

III. Demonstration of a seismometer response with amplitude and phase responses at:

III. Demonstration of a seismometer response with amplitude and phase responses at: GG5330, Spring semester 006 Assignment #1, Seismometry and Grond Motions De 30 Janary 006. 1. Calibration Of A Seismometer Using Java: A really nifty se of Java is now available for demonstrating the seismic

More information

Thermal balance of a wall with PCM-enhanced thermal insulation

Thermal balance of a wall with PCM-enhanced thermal insulation Thermal balance of a wall with PCM-enhanced thermal inslation E. Kossecka Institte of Fndamental Technological esearch of the Polish Academy of Sciences, Warsaw, Poland J. Kośny Oak idge National aboratory;

More information

Optimal Control of a Heterogeneous Two Server System with Consideration for Power and Performance

Optimal Control of a Heterogeneous Two Server System with Consideration for Power and Performance Optimal Control of a Heterogeneos Two Server System with Consideration for Power and Performance by Jiazheng Li A thesis presented to the University of Waterloo in flfilment of the thesis reqirement for

More information

Prandl established a universal velocity profile for flow parallel to the bed given by

Prandl established a universal velocity profile for flow parallel to the bed given by EM 0--00 (Part VI) (g) The nderlayers shold be at least three thicknesses of the W 50 stone, bt never less than 0.3 m (Ahrens 98b). The thickness can be calclated sing Eqation VI-5-9 with a coefficient

More information

WEAR PREDICTION OF A TOTAL KNEE PROSTHESIS TIBIAL TRAY

WEAR PREDICTION OF A TOTAL KNEE PROSTHESIS TIBIAL TRAY APPLIED PHYSICS MEDICAL WEAR PREDICTION OF A TOTAL KNEE PROSTHESIS TIBIAL TRAY L. CÃPITANU, A. IAROVICI, J. ONIªORU Institte of Solid Mechanics, Romanian Academy, Constantin Mille 5, Bcharest Received

More information

CONTENTS. INTRODUCTION MEQ curriculum objectives for vectors (8% of year). page 2 What is a vector? What is a scalar? page 3, 4

CONTENTS. INTRODUCTION MEQ curriculum objectives for vectors (8% of year). page 2 What is a vector? What is a scalar? page 3, 4 CONTENTS INTRODUCTION MEQ crriclm objectives for vectors (8% of year). page 2 What is a vector? What is a scalar? page 3, 4 VECTOR CONCEPTS FROM GEOMETRIC AND ALGEBRAIC PERSPECTIVES page 1 Representation

More information

Subsidence above a planar reservoir

Subsidence above a planar reservoir JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 17, NO. B9, 222, doi:1.129/21jb66, 22 Sbsidence above a planar reservoir J. B. Walsh Adamsville, Rhode Island, USA Received 9 May 21; revised 25 Janary 22; accepted

More information

Finite Difference Method of Modelling Groundwater Flow

Finite Difference Method of Modelling Groundwater Flow Jornal of Water Resorce and Protection, 20, 3, 92-98 doi:0.4236/warp.20.33025 Pblished Online March 20 (http://www.scirp.org/ornal/warp) Finite Difference Method of Modelling Grondwater Flow Abstract Magns.

More information

m = Average Rate of Change (Secant Slope) Example:

m = Average Rate of Change (Secant Slope) Example: Average Rate o Change Secant Slope Deinition: The average change secant slope o a nction over a particlar interval [a, b] or [a, ]. Eample: What is the average rate o change o the nction over the interval

More information

Restricted Three-Body Problem in Different Coordinate Systems

Restricted Three-Body Problem in Different Coordinate Systems Applied Mathematics 3 949-953 http://dx.doi.org/.436/am..394 Pblished Online September (http://www.scirp.org/jornal/am) Restricted Three-Body Problem in Different Coordinate Systems II-In Sidereal Spherical

More information

ECON3120/4120 Mathematics 2, spring 2009

ECON3120/4120 Mathematics 2, spring 2009 University of Oslo Department of Economics Arne Strøm ECON3/4 Mathematics, spring 9 Problem soltions for Seminar 4, 6 Febrary 9 (For practical reasons some of the soltions may inclde problem parts that

More information

Technical Note. ODiSI-B Sensor Strain Gage Factor Uncertainty

Technical Note. ODiSI-B Sensor Strain Gage Factor Uncertainty Technical Note EN-FY160 Revision November 30, 016 ODiSI-B Sensor Strain Gage Factor Uncertainty Abstract Lna has pdated or strain sensor calibration tool to spport NIST-traceable measrements, to compte

More information

sin u 5 opp } cos u 5 adj } hyp opposite csc u 5 hyp } sec u 5 hyp } opp Using Inverse Trigonometric Functions

sin u 5 opp } cos u 5 adj } hyp opposite csc u 5 hyp } sec u 5 hyp } opp Using Inverse Trigonometric Functions 13 Big Idea 1 CHAPTER SUMMARY BIG IDEAS Using Trigonometric Fnctions Algebra classzone.com Electronic Fnction Library For Yor Notebook hypotense acent osite sine cosine tangent sin 5 hyp cos 5 hyp tan

More information

Strategic Timing of Content in Online Social Networks

Strategic Timing of Content in Online Social Networks Strategic Timing of Content in Online Social Networks Sina Modaresi Department of Indstrial Engineering, University of Pittsbrgh, Pittsbrgh PA 56, sim3@pitt.ed Jan Pablo Vielma Sloan School of Management,

More information

Quantum Key Distribution Using Decoy State Protocol

Quantum Key Distribution Using Decoy State Protocol American J. of Engineering and Applied Sciences 2 (4): 694-698, 2009 ISSN 94-7020 2009 Science Pblications Qantm Key Distribtion sing Decoy State Protocol,2 Sellami Ali, 2 Shhairi Sahardin and,2 M.R.B.

More information

1 JAXA Special Pblication JAXA-SP-1-E Small-scale trblence affects flow fields arond a blff body and therefore it governs characteristics of cross-sec

1 JAXA Special Pblication JAXA-SP-1-E Small-scale trblence affects flow fields arond a blff body and therefore it governs characteristics of cross-sec First International Symposim on Fltter and its Application, 1 11 IEXPERIMENTAL STUDY ON TURBULENCE PARTIAL SIMULATION FOR BLUFF BODY Hiroshi Katschi +1 and Hitoshi Yamada + +1 Yokohama National University,

More information