Development of a Simplified Theoretical Model for Dynamic Burst Time And Pressure of a Cylindrical Shell

Size: px
Start display at page:

Download "Development of a Simplified Theoretical Model for Dynamic Burst Time And Pressure of a Cylindrical Shell"

Transcription

1 Te Open Ocean Engineeing Jounal 9 6 Open Access Developmen of a Simplified Teoeical Model fo Dynamic Bus Time And essue of a Cylindical Sell Cunjiang Ceng and G E Oo Widea Bjoksen Reseac Lab BIT 7 INC Madison Wisconsin Cene fo Joining and Manufacuing Assembly Mauee Univesiy Milwaukee Wisconsin Absac: Te objec of is sudy is o deemine e soem bus pessue and ime of meal cylindes unde soem dynamic loading condiions A simplified eoeical model o calculae ese dynamic bus ime and pessue of cylindical sells as been developed and e esuls ae compaed wi finie elemen analysis FEA esuls via e use of e LSDYNA code [] Based on e ageemen beween e wo esuls i can be concluded a a popely fomulaed simplified eoeical model can be employed wi sufficien accuacy o deemine e soem dynamic bus pessues of meal cylindes Keywods: Cylindical sell ipeline Dynamic bus pessue Dynamic bus ime INTRODUCTION Te cylindical sell is a basic sucue a is used all ove e wold in e sipping peocemical powe and aeospace indusies as well as in oes Envionmenal polluion popey damage pesonal injuy and even dea can occu wen a pessuied cylindical sell buss Teefoe an accuae deeminaion of e bus pessue of cylindical sells is a ciical paamee in e design pocess Consideable wok as been caied ou o deemine e saic bus pessue using eie analyical soluions expeimenal sudies o finie elemen analysis Dynamic loading suc as wae o seam amme penomena is also vey common in a pipeline o piping In e 95 s Coope [] developed an analyical euaion o pedic e saic bus pessue fo cylindes made of an isoopic ducile maeial Tis euaion povided e desied elaionsip beween e bus pessue maeial caaceisics oiginal dimensions and ulimae ensile seng of e maeial A e same ime Svensson [] deived a soluion of e bus pessue fo an abiay ick endcapped pipe based on e vonmises yield cieion Tadmo e al [4] developed an analyical expession of e bus pessue of mulilayeed cylindes Tey pefomed a lage sain analysis aking ino consideaion e elasicplasic defomaion wi e Hill yield funcion and abiay adening An oveall effecive modulus was used o deemine e onse of busing and ey en deived e elaions fo inwalled cylindes wi e neglec of e elasic sains Kleve [5] pesened an analyical model o deemine e bus seng of e inwall uncooded and cooded pipelines Te model esuls compaed well wi ose of an uncooded pipe es Sewa e al [6] eexamined e fundamenal elaionsips a goven e euilibium and sabiliy Addess coespondence o is auo a e Bjoksen Reseac Lab BIT 7 INC Madison Wisconsin; Tel: 68477; Fax: ; cengcunjiang@gmailcom geowidea@muedu 87485X9 of a pipe unde inceasing inenal pessue Bo Tesca s and vonmises yield cieia wee consideed Te auos concluded a ei analyical model is suiable fo bo in and ickwall cases Adaci e al [7] poposed a maemaical soluion fo pipe elasic sess based on e assumpion of onedimensional popagaion of e pessue and e uasisaic defomaion of e pipe o calculae e elasic sesses in a ube due o wae amme Leisea e al [8] pesened bo an analyical soluion and a finie elemen analysis o deemine e dynamic pipe sess due o e vibaions ceaed by wae amme wi e assumpions a e maeial is linealy elasic and e wae amme load as been limied o a sep pessue incease insead of a amped pessue incease He concluded a e maximum dynamic sess is wice a of e saic sess wen damping is ignoed Neie Adaci no Leisea consideed dynamic plasic defomaion Only a limied amoun wok as been publised o deemine e dynamic elasic sess in pipes bu no lieaue is available on e dynamic bus pessue of cylindical sells SIMLIFIED THEORETICAL MODEL To make easily undesand e effec of facos suc as e pessue vs ime funcion and e diamee vs ickness aio on e bus pessue as well as examine e consisency of e FEA esuls a eoeical analysis meod based on a simplified inwalled cylinde geomey is developed Conside a inwalled axisymmeic cylinde unde unifom dynamic inenal pessue Te geomey and beavio of is cylinde can be descibed by use of cylindical coodinaes Assume plane sain beavio Assume fue a e oop sess is e dominan sess and a i can be aken o be consan ougou e ickness of e cylinde Wi efeence o Fig e summaion of foces in e adial diecion fo an elemen of volume 9 Benam Open d dl is

2 Te Open Ocean Engineeing Jounal 9 Volume Ceng and Widea dθ dl 8 o σ dθ 9 Fig Simplified Geomey and Loading Condiion of Cylinde d dl d dl sin F Assume a e mass of is small volume of e cylinde will emain consan; i can eefoe be expessed as m d dl In e above is e insananeous wall ickness e iniial wall ickness dl e incemen of cylinde leng e densiy e insananeous inside adius e iniial inside adius and d e small incemen in ac angle Define e adial acceleaion in a d d a as Wen d is vey small e euaion 4 can be esablised d d sin Because e cylinde is assumed o be inwalled e acceleaion can be aken o be consan ougou e ickness Te euaion of moion in e adical diecion fo e volume elemen can us be wien as d d dl dl d dl 5 Te assumpion of volume consancy duing e defomaion pocess saisfies e following euaion: wic yields dl Euaion 5 can now be wien as 4 dl 6 7 Fo a vey small incemen of e adial sain one can wie d d One can inegae bo side of e euaion and obain d ln ln wic yields e Wi a consideaion of e exisence of sain ae effecs e following euaion can be developed o fi e maeial daa elaing sess sain and sain ae cuves by using MaCAD [] sofwae: n k D Hee is e effecive vonmises sess and e effecive vonmises sain Fue k and n ae consans fo a paicula maeial Te assumpion of volume consancy duing e defomaion also leads o e following euaion: 4 Fo plane sain and us 5 Te effecive vonmises sain is defined by e following euaion: 6 Fo plane sain i becomes 7

3 Developmen of a Simplified Teoeical Model Te Open Ocean Engineeing Jounal 9 Volume Fo a inwalled cylinde adius is muc lage an e ickness and e adial sess is small compaed o e oe wo sesses Teefoe one can assume 8 Also 9 Te effecive vonmises sess is defined by e following euaion: Wi e assumpions made is expession can be solved fo and becomes 4 k n D Euaing e euaion o e euaion 9 one obains Subsiuing euaions 7 7 and 9 ino e euaion esuls in: Hee ln ln Te mos geneal appoac fo e soluion of e dynamic esponse of sucual sysems is e diec numeical inegaion of e dynamic euilibium euaions Euaion is a vey complicaed diffeenial euaion based on e vaiable I canno be solved diecly by using e egula cenal diffeence meod o e Newmak meod [] Hee a simila explici numeical meod is developed based on e geneal cenal diffeence meod Tus 4 Combine e expessions of 4 wi e euaion o obain e euaion 5: eoeically one can solve e euaion 5 using e iniial condiions of and Hee is e known iniial inside adius Radius can be solved fom following euaions: D k n 4 4 k n D

4 4 Te Open Ocean Engineeing Jounal 9 Volume Ceng and Widea p 4 k ln n D ln p Combining euaions 6 and 7 wi e euaion 5 one obains euaion 8: Table ASTM A6B Maeial Descipion Cemical Analysis C Mn S Si Ω Condiion Seamless oolled In e sample calculaion e cylindical sell as an ouside diamee of 4 inces and a wall ickness of 65 4 k ln n D ln 8 In euaion 8 e only unknown vaiable is Teefoe eoeically i is solvable Howeve due o e ig nonlineaiy i is difficul o solve is euaion manually Euaion 8 and en euaion 5 can be solved using a commecial maemaics sofwae suc as MaCAD [] To make sue a e euaion 5 is always solvable e incemenal ime sep sould be vey small Howeve wen e ime sep is smalle an e minimum pecision of e MaCAD sofwae e soluion will be unsable A sample calculaion is pefomed by using MaCAD Te maeial is ASTM6 seel [] Te maeial descipion is lised in Table Te sess sain and sain ae cuves ae sown in Fig By fiing e sess sain and sain ae cuves one can ge e maeial coefficiens of k n and Te pessue vs ime cuve is aken as e amped cuve sown in Fig Hee e ime d is pessue pulse duaion Sess E9 a Sess Sain Cuves a Diffeen Sain Raes Sain mmmm Saic Es Sain Rae 4Es Sain Rae 48Es Sain Rae Fig Sesssain Cuve of A6B Seel a Diffeen Sain Raes

5 Developmen of a Simplified Teoeical Model Te Open Ocean Engineeing Jounal 9 Volume 5 d d Fig essue psi vs Time second Cuve Fixed Symmeic Dynamic essue Inside Fig 4 FEA Model Loading and Bounday Condiions inces Te esuling bus ime is abou milliseconds wen e peak pessue is psi To confim ese calculaions a finie elemen analysis FEA is caied ou using e dynamic compue code LS DYNA [] In developing e FEA mes e eig node solid elemen is employed and e guidelines saed in efeence [4] ae followed In paicula e mes as ee elemens acoss e ickness see Fig 5 and e elemen sie is 97 in Te bounday condiions and loading see Fig 4 ae as follows: One end is fixed e oe end is fee Dynamic Foce Inenal pessue is a funcion of ime see Fig wi e maximum ampliude aken as 5 8 Fig 5 FEA Mes 76 and 7 psi A dynamic foce eual o e pessue muliplied by e inside aea of e cylinde is added a e fee end Gaviy acs along e Y axis In e FEA simulaion e bus cieion is based on e maximum plasic sain a diffeen sain aes Once e plasic sain of an elemen eaces e maximum plasic sain fo a ceain sain ae e elemen is deleed fom e calculaion Te bus pessue and ime can be ecoded fom e oupu of e FEA model Moe deailed seup mes esuls and configuaions can be found in efeence [5] Table clealy sows a e bus pessue pediced by FEA is 8 psi wile a pediced by eoeical meod is 76 psi fo e cylinde unde consideaion Te bus imes ae close as well SUMMARY A simplified explici numeical meod o calculae e dynamic bus pessue and ime of a inwalled cylindical sell is developed A sample esul fom e use of is meod is compaed wi FEA esuls and i is sown a e pesen simplified eoeical meod can be used o accuaely deemine e bus pessue and ime of a inwalled cylindical sell Table Compaison of Euaion and FEA Resuls OD inc Tickness inc d ms eak essue psi FEA Bus Time ms Euaion Bus Time ms No bus No bus No bus

6 6 Te Open Ocean Engineeing Jounal 9 Volume Ceng and Widea REFERENCES [] LSDYNA Teoeical manual Livemoe Sofwae Tecnology Copoaion 998 [] WE Coope Te significance of e ensile es o pessue vessel design Welding Reseac Supplemen pp 4956 Jan 957 [] NL Svensson Bus pessue of cylindical and speical vessels Jounal of Applied Mecanics vol 5 No pp [4] EB Tadmo and D Duban lasic defomaion and bus of pessuied mulilayeed cylindes Jounal of essue Vessel Tecnology vol 7 pp 859 Feb 995 [5] FJ Kleve Bus seng of cooded pipe: flow sess evisied Twenyfou annual Offsoe Tecnology Confeence May 47 Houson Texas 99 [6] G Sewa and FJ Kleve An analyical model o pedic e bus capabiliy of pipelines Inenaional Confeence on Offsoe Mecanics and Acic Engineeing vol 5 Houson Texas ipeline Tecnology 994 [7] T Adaci S Ujiasi and H Masumoo Impulsive esponses of a cicula cylinde sell subjec o wae amme waves Jounal of essue Vessel Tecnology vol pp 575 Nov 99 [8] RA Leisea CA Young and E M Alfod Dynamic pipe sesses duing wae amme I finie elemen appoac Design and Analysis of iping Vessels and Componens ASME essue Vessels and iping Confeence Vancouve: Biis Columbia Canada Augus 59 [9] RA Leisea Dynamic pipe sesses duing wae amme II a vibaion analysis Design and analysis of piping vessels and componens ASME essue Vessels and iping Confeence Vancouve: Biis Columbia Canada Augus 59 [] RA Leisea Dynamic pipe sesses duing wae amme III complex sesses Design and analysis of piping vessels and componens ASME essue Vessels and iping Confeence Vancouve: Biis Columbia Canada Augus 59 [] MaCAD Use s Guide Masof Engineeing Educaion Inc Cambidge MA USA 5 [] NM Newmak A meod of compuaion fo sucual dynamics Jounal of Engineeing Mecanics Division ASCE EM vol 85 pp [] D eeson ipe wip dynamics: an expeimenal and analyical invesigaion D Disseaion Univesiy of Akon 98 [4] GEO Widea and L Xue Guidelines fo FEA fodeling of cylindeocylinde Inesecions WRC Bullein No 49 New Yok: Welding Reseac Council 4 [5] C Ceng and GEO Widea Dynamic bus pessue simulaion of cylindical sells in oceedings of e 8 ASME essue Vessels iping Confeence Cicago IL USA July 7 8 Received: June 8 Revised: Januay 9 Acceped: Januay 9 Ceng and Widea; Licensee Benam Open Tis is an open access aicle licensed unde e ems of e Ceaive Commons Aibuion NonCommecial License p:ceaivecommonsoglicensesbync wic pemis unesiced noncommecial use disibuion and epoducion in any medium povided e wok is popely cied

Heat Conduction Problem in a Thick Circular Plate and its Thermal Stresses due to Ramp Type Heating

Heat Conduction Problem in a Thick Circular Plate and its Thermal Stresses due to Ramp Type Heating ISSN(Online): 319-8753 ISSN (Pin): 347-671 Inenaional Jounal of Innovaive Reseac in Science, Engineeing and Tecnology (An ISO 397: 7 Ceified Oganiaion) Vol 4, Issue 1, Decembe 15 Hea Concion Poblem in

More information

NUMERICAL SIMULATION FOR NONLINEAR STATIC & DYNAMIC STRUCTURAL ANALYSIS

NUMERICAL SIMULATION FOR NONLINEAR STATIC & DYNAMIC STRUCTURAL ANALYSIS Join Inenaional Confeence on Compuing and Decision Making in Civil and Building Engineeing June 14-16, 26 - Monéal, Canada NUMERICAL SIMULATION FOR NONLINEAR STATIC & DYNAMIC STRUCTURAL ANALYSIS ABSTRACT

More information

MEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING

MEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING MEEN 67 Handou # MODAL ANALYSIS OF MDOF Sysems wih VISCOS DAMPING ^ Symmeic Moion of a n-dof linea sysem is descibed by he second ode diffeenial equaions M+C+K=F whee () and F () ae n ows vecos of displacemens

More information

Elastic-Plastic Deformation of a Rotating Solid Disk of Exponentially Varying Thickness and Exponentially Varying Density

Elastic-Plastic Deformation of a Rotating Solid Disk of Exponentially Varying Thickness and Exponentially Varying Density Poceedings of he Inenaional MuliConfeence of Enginees Compue Scieniss 6 Vol II, IMECS 6, Mach 6-8, 6, Hong Kong Elasic-Plasic Defomaion of a Roaing Solid Dis of Exponenially Vaying hicness Exponenially

More information

Combinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions

Combinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions Inenaional Mahemaical Foum, Vol 8, 03, no 0, 463-47 HIKARI Ld, wwwm-hikaicom Combinaoial Appoach o M/M/ Queues Using Hypegeomeic Funcions Jagdish Saan and Kamal Nain Depamen of Saisics, Univesiy of Delhi,

More information

Orthotropic Materials

Orthotropic Materials Kapiel 2 Ohoopic Maeials 2. Elasic Sain maix Elasic sains ae elaed o sesses by Hooke's law, as saed below. The sesssain elaionship is in each maeial poin fomulaed in he local caesian coodinae sysem. ε

More information

Monochromatic Wave over One and Two Bars

Monochromatic Wave over One and Two Bars Applied Mahemaical Sciences, Vol. 8, 204, no. 6, 307-3025 HIKARI Ld, www.m-hikai.com hp://dx.doi.og/0.2988/ams.204.44245 Monochomaic Wave ove One and Two Bas L.H. Wiyano Faculy of Mahemaics and Naual Sciences,

More information

Lecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain

Lecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain Lecue-V Sochasic Pocesses and he Basic Tem-Sucue Equaion 1 Sochasic Pocesses Any vaiable whose value changes ove ime in an unceain way is called a Sochasic Pocess. Sochasic Pocesses can be classied as

More information

Pressure Vessels Thin and Thick-Walled Stress Analysis

Pressure Vessels Thin and Thick-Walled Stress Analysis Pessue Vessels Thin and Thick-Walled Sess Analysis y James Doane, PhD, PE Conens 1.0 Couse Oveview... 3.0 Thin-Walled Pessue Vessels... 3.1 Inoducion... 3. Sesses in Cylindical Conaines... 4..1 Hoop Sess...

More information

The sudden release of a large amount of energy E into a background fluid of density

The sudden release of a large amount of energy E into a background fluid of density 10 Poin explosion The sudden elease of a lage amoun of enegy E ino a backgound fluid of densiy ceaes a song explosion, chaaceized by a song shock wave (a blas wave ) emanaing fom he poin whee he enegy

More information

Overview. Overview Page 1 of 8

Overview. Overview Page 1 of 8 COMPUTERS AND STRUCTURES, INC., BERKELEY, CALIORNIA DECEMBER 2001 COMPOSITE BEAM DESIGN AISC-LRD93 Tecnical Noe Compac and Noncompac Requiemens Tis Tecnical Noe descibes o e pogam cecks e AISC-LRD93 specificaion

More information

Chapter Finite Difference Method for Ordinary Differential Equations

Chapter Finite Difference Method for Ordinary Differential Equations Chape 8.7 Finie Diffeence Mehod fo Odinay Diffeenial Eqaions Afe eading his chape, yo shold be able o. Undesand wha he finie diffeence mehod is and how o se i o solve poblems. Wha is he finie diffeence

More information

Lecture 22 Electromagnetic Waves

Lecture 22 Electromagnetic Waves Lecue Elecomagneic Waves Pogam: 1. Enegy caied by he wave (Poyning veco).. Maxwell s equaions and Bounday condiions a inefaces. 3. Maeials boundaies: eflecion and efacion. Snell s Law. Quesions you should

More information

MECHANICS OF MATERIALS Poisson s Ratio

MECHANICS OF MATERIALS Poisson s Ratio Fouh diion MCHANICS OF MATRIALS Poisson s Raio Bee Johnson DeWolf Fo a slende ba subjeced o aial loading: 0 The elongaion in he -diecion is accompanied b a conacion in he ohe diecions. Assuming ha he maeial

More information

KINEMATICS OF RIGID BODIES

KINEMATICS OF RIGID BODIES KINEMTICS OF RIGID ODIES In igid body kinemaics, we use he elaionships govening he displacemen, velociy and acceleaion, bu mus also accoun fo he oaional moion of he body. Descipion of he moion of igid

More information

STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE WEIBULL DISTRIBUTION

STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE WEIBULL DISTRIBUTION Inenaional Jounal of Science, Technology & Managemen Volume No 04, Special Issue No. 0, Mach 205 ISSN (online): 2394-537 STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE

More information

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion

More information

General Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security

General Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security 1 Geneal Non-Abiage Model I. Paial Diffeenial Equaion fo Picing A. aded Undelying Secuiy 1. Dynamics of he Asse Given by: a. ds = µ (S, )d + σ (S, )dz b. he asse can be eihe a sock, o a cuency, an index,

More information

Lecture 17: Kinetics of Phase Growth in a Two-component System:

Lecture 17: Kinetics of Phase Growth in a Two-component System: Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien

More information

, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t

, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t Lecue 6: Fiis Tansmission Equaion and Rada Range Equaion (Fiis equaion. Maximum ange of a wieless link. Rada coss secion. Rada equaion. Maximum ange of a ada. 1. Fiis ansmission equaion Fiis ansmission

More information

Fluid Flow and Heat Transfer Characteristics across an Internally Heated Finned Duct

Fluid Flow and Heat Transfer Characteristics across an Internally Heated Finned Duct J. Enegy Powe Souces ol. No. 6 4 pp. 96-33 ceived: Augus 3 4 Published: Decembe 3 4 Jounal of Enegy and Powe Souces www.ehanpublishing.com Fluid Flow and ea ansfe Chaaceisics acoss an Inenally eaed Finned

More information

Theoretical background and the flow fields in downhole liquid-liquid hydrocyclone (LLHC)

Theoretical background and the flow fields in downhole liquid-liquid hydrocyclone (LLHC) AEC Web of Confeences 13, 3 (14) DO: 1.151/ maecconf/ 1413 3 C Owned by he auhos, published by EDP Sciences, 14 heoeical backgound and he flow fields in downhole liquid-liquid hydocyclone (LLHC) Haison

More information

Low-complexity Algorithms for MIMO Multiplexing Systems

Low-complexity Algorithms for MIMO Multiplexing Systems Low-complexiy Algoihms fo MIMO Muliplexing Sysems Ouline Inoducion QRD-M M algoihm Algoihm I: : o educe he numbe of suviving pahs. Algoihm II: : o educe he numbe of candidaes fo each ansmied signal. :

More information

Efficient experimental detection of milling stability boundary and the optimal axial immersion for helical mills

Efficient experimental detection of milling stability boundary and the optimal axial immersion for helical mills Efficien expeimenal deecion of milling sabiliy bounday and he opimal axial immesion fo helical mills Daniel BACHRATHY Depamen of Applied Mechanics, Budapes Univesiy of Technology and Economics Muegyeem

More information

A Strain Based Design Criterion for Solid Propellant Rocket Motors

A Strain Based Design Criterion for Solid Propellant Rocket Motors Robe NEVIERE, Fancine STANKIEWICZ SNPE Cene de Recheches du BOUCHET BP, 97 Ve-le-Pei FRANCE Andé PFIFFER CELERG Eablissemen de S MEDARD BP, 65 S MEDARD-en-JALLES FRANCE. INTRODUCTION Due o a quie complex

More information

Numerical solution of fuzzy differential equations by Milne s predictor-corrector method and the dependency problem

Numerical solution of fuzzy differential equations by Milne s predictor-corrector method and the dependency problem Applied Maemaics and Sciences: An Inenaional Jounal (MaSJ ) Vol. No. Augus 04 Numeical soluion o uzz dieenial equaions b Milne s pedico-coeco meod and e dependenc poblem Kanagaajan K Indakuma S Muukuma

More information

Two-dimensional Effects on the CSR Interaction Forces for an Energy-Chirped Bunch. Rui Li, J. Bisognano, R. Legg, and R. Bosch

Two-dimensional Effects on the CSR Interaction Forces for an Energy-Chirped Bunch. Rui Li, J. Bisognano, R. Legg, and R. Bosch Two-dimensional Effecs on he CS Ineacion Foces fo an Enegy-Chiped Bunch ui Li, J. Bisognano,. Legg, and. Bosch Ouline 1. Inoducion 2. Pevious 1D and 2D esuls fo Effecive CS Foce 3. Bunch Disibuion Vaiaion

More information

Probabilistic Models. CS 188: Artificial Intelligence Fall Independence. Example: Independence. Example: Independence? Conditional Independence

Probabilistic Models. CS 188: Artificial Intelligence Fall Independence. Example: Independence. Example: Independence? Conditional Independence C 188: Aificial Inelligence Fall 2007 obabilisic Models A pobabilisic model is a join disibuion ove a se of vaiables Lecue 15: Bayes Nes 10/18/2007 Given a join disibuion, we can eason abou unobseved vaiables

More information

Circular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can.

Circular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can. 1 Cicula Moion Radians One evoluion is equivalen o 360 0 which is also equivalen o 2π adians. Theefoe we can say ha 360 = 2π adians, 180 = π adians, 90 = π 2 adians. Hence 1 adian = 360 2π Convesions Rule

More information

PHYS PRACTICE EXAM 2

PHYS PRACTICE EXAM 2 PHYS 1800 PRACTICE EXAM Pa I Muliple Choice Quesions [ ps each] Diecions: Cicle he one alenaive ha bes complees he saemen o answes he quesion. Unless ohewise saed, assume ideal condiions (no ai esisance,

More information

Pseudosteady-State Flow Relations for a Radial System from Department of Petroleum Engineering Course Notes (1997)

Pseudosteady-State Flow Relations for a Radial System from Department of Petroleum Engineering Course Notes (1997) Pseudoseady-Sae Flow Relaions fo a Radial Sysem fom Deamen of Peoleum Engineeing Couse Noes (1997) (Deivaion of he Pseudoseady-Sae Flow Relaions fo a Radial Sysem) (Deivaion of he Pseudoseady-Sae Flow

More information

On Control Problem Described by Infinite System of First-Order Differential Equations

On Control Problem Described by Infinite System of First-Order Differential Equations Ausalian Jounal of Basic and Applied Sciences 5(): 736-74 ISS 99-878 On Conol Poblem Descibed by Infinie Sysem of Fis-Ode Diffeenial Equaions Gafujan Ibagimov and Abbas Badaaya J'afau Insiue fo Mahemaical

More information

FINITE DIFFERENCE APPROACH TO WAVE GUIDE MODES COMPUTATION

FINITE DIFFERENCE APPROACH TO WAVE GUIDE MODES COMPUTATION FINITE DIFFERENCE ROCH TO WVE GUIDE MODES COMUTTION Ing.lessando Fani Elecomagneic Gou Deamen of Elecical and Eleconic Engineeing Univesiy of Cagliai iazza d mi, 93 Cagliai, Ialy SUMMRY Inoducion Finie

More information

r P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2 " P 1 = " #P L L,

r P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2  P 1 =  #P L L, Lecue 36 Pipe Flow and Low-eynolds numbe hydodynamics 36.1 eading fo Lecues 34-35: PKT Chape 12. Will y fo Monday?: new daa shee and daf fomula shee fo final exam. Ou saing poin fo hydodynamics ae wo equaions:

More information

Research Article Stress Analysis of Nonhomogeneous Rotating Disc with Arbitrarily Variable Thickness Using Finite Element Method

Research Article Stress Analysis of Nonhomogeneous Rotating Disc with Arbitrarily Variable Thickness Using Finite Element Method Reseach Jounal of Applied Sciences, Engineeing and Technology 7(15): 3114-315, 014 DOI:10.1906/jase.7.650 ISSN: 040-7459; e-issn: 040-7467 014 Maxwell Scienific Publicaion Cop. Submied: Ocobe 09, 013 Acceped:

More information

Computer Propagation Analysis Tools

Computer Propagation Analysis Tools Compue Popagaion Analysis Tools. Compue Popagaion Analysis Tools Inoducion By now you ae pobably geing he idea ha pedicing eceived signal sengh is a eally impoan as in he design of a wieless communicaion

More information

CONSIDERATIONS REGARDING THE OPTIMUM DESIGN OF PRESTRESSED ELEMENTS

CONSIDERATIONS REGARDING THE OPTIMUM DESIGN OF PRESTRESSED ELEMENTS Bullein of e Transilvania Universiy of Braşov CIBv 5 Vol. 8 (57) Special Issue No. - 5 CONSIDERTIONS REGRDING THE OPTIU DESIGN OF PRESTRESSED ELEENTS D. PRECUPNU C. PRECUPNU bsrac: Engineering educaion

More information

Process model for the design of bent 3-dimensional free-form geometries for the three-roll-push-bending process

Process model for the design of bent 3-dimensional free-form geometries for the three-roll-push-bending process Available online a www.sciencediec.com Pocedia CIRP 7 (213 ) 24 245 Foy Sixh CIRP Confeence on Manufacuing Sysems 213 Pocess model fo he design of ben 3-dimensional fee-fom geomeies fo he hee-oll-push-bending

More information

Today - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations

Today - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy

More information

ME 304 FLUID MECHANICS II

ME 304 FLUID MECHANICS II ME 304 LUID MECHNICS II Pof. D. Haşme Tükoğlu Çankaya Uniesiy aculy of Engineeing Mechanical Engineeing Depamen Sping, 07 y du dy y n du k dy y du k dy n du du dy dy ME304 The undamenal Laws Epeience hae

More information

7 Wave Equation in Higher Dimensions

7 Wave Equation in Higher Dimensions 7 Wave Equaion in Highe Dimensions We now conside he iniial-value poblem fo he wave equaion in n dimensions, u c u x R n u(x, φ(x u (x, ψ(x whee u n i u x i x i. (7. 7. Mehod of Spheical Means Ref: Evans,

More information

Design Guideline for Buried Hume Pipe Subject to Coupling Forces

Design Guideline for Buried Hume Pipe Subject to Coupling Forces Design Guideline fo Buied Hume Pipe Sujec o Coupling Foces Won Pyo Hong 1), *Seongwon Hong 2), and Thomas Kang 3) 1) Depamen of Civil, nvionmenal and Plan ngineeing, Chang-Ang Univesiy, Seoul 06974, Koea

More information

MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH

MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Fundamenal Jounal of Mahemaical Phsics Vol 3 Issue 013 Pages 55-6 Published online a hp://wwwfdincom/ MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Univesias

More information

CS 188: Artificial Intelligence Fall Probabilistic Models

CS 188: Artificial Intelligence Fall Probabilistic Models CS 188: Aificial Inelligence Fall 2007 Lecue 15: Bayes Nes 10/18/2007 Dan Klein UC Bekeley Pobabilisic Models A pobabilisic model is a join disibuion ove a se of vaiables Given a join disibuion, we can

More information

Control Volume Derivation

Control Volume Derivation School of eospace Engineeing Conol Volume -1 Copyigh 1 by Jey M. Seizman. ll ighs esee. Conol Volume Deiaion How o cone ou elaionships fo a close sysem (conol mass) o an open sysem (conol olume) Fo mass

More information

ÖRNEK 1: THE LINEAR IMPULSE-MOMENTUM RELATION Calculate the linear momentum of a particle of mass m=10 kg which has a. kg m s

ÖRNEK 1: THE LINEAR IMPULSE-MOMENTUM RELATION Calculate the linear momentum of a particle of mass m=10 kg which has a. kg m s MÜHENDİSLİK MEKANİĞİ. HAFTA İMPULS- MMENTUM-ÇARPIŞMA Linea oenu of a paicle: The sybol L denoes he linea oenu and is defined as he ass ies he elociy of a paicle. L ÖRNEK : THE LINEAR IMPULSE-MMENTUM RELATIN

More information

Chapter 7. Interference

Chapter 7. Interference Chape 7 Inefeence Pa I Geneal Consideaions Pinciple of Supeposiion Pinciple of Supeposiion When wo o moe opical waves mee in he same locaion, hey follow supeposiion pinciple Mos opical sensos deec opical

More information

AN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS

AN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS AN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS M. KAMESWAR RAO AND K.P. RAVINDRAN Depamen of Mechanical Engineeing, Calicu Regional Engineeing College, Keala-67 6, INDIA. Absac:- We eploe

More information

Additional Exercises for Chapter What is the slope-intercept form of the equation of the line given by 3x + 5y + 2 = 0?

Additional Exercises for Chapter What is the slope-intercept form of the equation of the line given by 3x + 5y + 2 = 0? ddiional Eercises for Caper 5 bou Lines, Slopes, and Tangen Lines 39. Find an equaion for e line roug e wo poins (, 7) and (5, ). 4. Wa is e slope-inercep form of e equaion of e line given by 3 + 5y +

More information

The Production of Polarization

The Production of Polarization Physics 36: Waves Lecue 13 3/31/211 The Poducion of Polaizaion Today we will alk abou he poducion of polaized ligh. We aleady inoduced he concep of he polaizaion of ligh, a ansvese EM wave. To biefly eview

More information

Q & Particle-Gas Multiphase Flow. Particle-Gas Interaction. Particle-Particle Interaction. Two-way coupling fluid particle. Mass. Momentum.

Q & Particle-Gas Multiphase Flow. Particle-Gas Interaction. Particle-Particle Interaction. Two-way coupling fluid particle. Mass. Momentum. Paicle-Gas Muliphase Flow Fluid Mass Momenum Enegy Paicles Q & m& F D Paicle-Gas Ineacion Concenaion highe dilue One-way coupling fluid paicle Two-way coupling fluid paicle Concenaion highe Paicle-Paicle

More information

WORK POWER AND ENERGY Consevaive foce a) A foce is said o be consevaive if he wok done by i is independen of pah followed by he body b) Wok done by a consevaive foce fo a closed pah is zeo c) Wok done

More information

A New Mathematical Approach to the Turbulence Closure Problem

A New Mathematical Approach to the Turbulence Closure Problem Ameican Jounal of Fluid Dynamics 6, 6(: 7-4 DOI: 93/j.ajfd.66 A New Mahemaical Appoach o he Tubulence Closue Poblem Mohammed A. Azim Depamen of Mechanical Engineeing, Bangladesh Univesiy of Engineeing

More information

LawsoftheElectroElectricalInduction

LawsoftheElectroElectricalInduction Global Jounal of Reseaches in Engineeing: F Elecical and Eleconics Engineeing Volume 15 Issue 9 Vesion 1. Yea 15 Type: Double Blind Pee Reviewed Inenaional Reseach Jounal Publishe: Global Jounals Inc.

More information

Determination of Stresses in Drying Wood by Means of a Viscoelastic Relaxation Model

Determination of Stresses in Drying Wood by Means of a Viscoelastic Relaxation Model Deeminaion of Sesses in Dying Wood by Means of a Viscoelasic Relaxaion Model Oma Saifouni, Rosand Mouou Pii, Jean-Fançois Desebecq To cie his vesion: Oma Saifouni, Rosand Mouou Pii, Jean-Fançois Desebecq.

More information

A Numerical Hydration Model of Portland Cement

A Numerical Hydration Model of Portland Cement A Numeical Hydaion Model of Poland Cemen Ippei Mauyama, Tesuo Masushia and Takafumi Noguchi ABSTRACT : A compue-based numeical model is pesened, wih which hydaion and micosucual developmen in Poland cemen-based

More information

Comparison between the Discrete and Continuous Time Models

Comparison between the Discrete and Continuous Time Models Comparison beween e Discree and Coninuous Time Models D. Sulsky June 21, 2012 1 Discree o Coninuous Recall e discree ime model Î = AIS Ŝ = S Î. Tese equaions ell us ow e populaion canges from one day o

More information

Modelling Hydromechanical Dilation Geomaterial Cavitation and Localization

Modelling Hydromechanical Dilation Geomaterial Cavitation and Localization Modelling Hydomechanical Dilaion Geomaeial Caviaion and Localizaion Y. Sieffe, O. Buzzi, F. Collin and R. Chambon Absac This pape pesens an exension of he local second gadien model o muliphasic maeials

More information

Sections 3.1 and 3.4 Exponential Functions (Growth and Decay)

Sections 3.1 and 3.4 Exponential Functions (Growth and Decay) Secions 3.1 and 3.4 Eponenial Funcions (Gowh and Decay) Chape 3. Secions 1 and 4 Page 1 of 5 Wha Would You Rahe Have... $1million, o double you money evey day fo 31 days saing wih 1cen? Day Cens Day Cens

More information

AST1100 Lecture Notes

AST1100 Lecture Notes AST00 Lecue Noes 5 6: Geneal Relaiviy Basic pinciples Schwazschild geomey The geneal heoy of elaiviy may be summaized in one equaion, he Einsein equaion G µν 8πT µν, whee G µν is he Einsein enso and T

More information

An Automatic Door Sensor Using Image Processing

An Automatic Door Sensor Using Image Processing An Auomaic Doo Senso Using Image Pocessing Depamen o Elecical and Eleconic Engineeing Faculy o Engineeing Tooi Univesiy MENDEL 2004 -Insiue o Auomaion and Compue Science- in BRNO CZECH REPUBLIC 1. Inoducion

More information

International Journal of Pure and Applied Sciences and Technology

International Journal of Pure and Applied Sciences and Technology In. J. Pue Appl. Sci. Technol., 4 (211, pp. 23-29 Inenaional Jounal of Pue and Applied Sciences and Technology ISS 2229-617 Available online a www.ijopaasa.in eseach Pape Opizaion of he Uiliy of a Sucual

More information

Variance and Covariance Processes

Variance and Covariance Processes Vaiance and Covaiance Pocesses Pakash Balachandan Depamen of Mahemaics Duke Univesiy May 26, 2008 These noes ae based on Due s Sochasic Calculus, Revuz and Yo s Coninuous Maingales and Bownian Moion, Kaazas

More information

Physics 2001/2051 Moments of Inertia Experiment 1

Physics 2001/2051 Moments of Inertia Experiment 1 Physics 001/051 Momens o Ineia Expeimen 1 Pelab 1 Read he ollowing backgound/seup and ensue you ae amilia wih he heoy equied o he expeimen. Please also ill in he missing equaions 5, 7 and 9. Backgound/Seup

More information

Stress Analysis of Infinite Plate with Elliptical Hole

Stress Analysis of Infinite Plate with Elliptical Hole Sess Analysis of Infinie Plae ih Ellipical Hole Mohansing R Padeshi*, D. P. K. Shaa* * ( P.G.Suden, Depaen of Mechanical Engg, NRI s Insiue of Infoaion Science & Technology, Bhopal, India) * ( Head of,

More information

Dynamic Operational Optimization of Air Source Heat Pump Heating System with the Consideration of Energy Saving

Dynamic Operational Optimization of Air Source Heat Pump Heating System with the Consideration of Energy Saving Pepins of he 9h Inenaional Symposium on Advanced Conol of Chemical Pocesses The Inenaional Fedeaion of Auomaic Conol June 7-1, 15, Whisle, Biish Columbia, Canada TuA.6 Dynamic Opeaional Opimiaion of Ai

More information

Prediction of Tank Fuel Sloshing during Jettison

Prediction of Tank Fuel Sloshing during Jettison Andé Baeen EADS, Miliay Aicaf, 8 Munic, Gemany ande.baeen@m.eads.ne Rupe Gleissl EADS, Miliay Aicaf, 8 Munic, Gemany upe.gleissl@m.eads.ne ABSTRACT Sepaaion Cleaances fo anks povide in geneal e mos limiing

More information

An S-type singular value inclusion set for rectangular tensors

An S-type singular value inclusion set for rectangular tensors Sang Jounal of Inequaliies and Applicaions 2017) 2017:141 DOI 10.1186/s13660-017-1421-0 R E S E A R C H Open Access An S-ype singula value inclusion se fo ecangula ensos Caili Sang * * Coespondence: sangcl@126.com

More information

Thermal-Fluids I. Chapter 17 Steady heat conduction. Dr. Primal Fernando Ph: (850)

Thermal-Fluids I. Chapter 17 Steady heat conduction. Dr. Primal Fernando Ph: (850) emal-fluids I Capte 7 Steady eat conduction D. Pimal Fenando pimal@eng.fsu.edu P: (850 40-633 Steady eat conduction Hee we conside one dimensional steady eat conduction. We conside eat tansfe in a plane

More information

Fundamental Vehicle Loads & Their Estimation

Fundamental Vehicle Loads & Their Estimation Fundaenal Vehicle Loads & Thei Esiaion The silified loads can only be alied in he eliinay design sage when he absence of es o siulaion daa They should always be qualified and udaed as oe infoaion becoes

More information

The Global Trade and Environment Model: GTEM

The Global Trade and Environment Model: GTEM The Global Tade and Envionmen Model: A pojecion of non-seady sae daa using Ineempoal GTEM Hom Pan, Vivek Tulpulé and Bian S. Fishe Ausalian Bueau of Agiculual and Resouce Economics OBJECTIVES Deive an

More information

Sharif University of Technology - CEDRA By: Professor Ali Meghdari

Sharif University of Technology - CEDRA By: Professor Ali Meghdari Shaif Univesiy of echnology - CEDRA By: Pofesso Ali Meghai Pupose: o exen he Enegy appoach in eiving euaions of oion i.e. Lagange s Meho fo Mechanical Syses. opics: Genealize Cooinaes Lagangian Euaion

More information

The shortest path between two truths in the real domain passes through the complex domain. J. Hadamard

The shortest path between two truths in the real domain passes through the complex domain. J. Hadamard Complex Analysis R.G. Halbud R.Halbud@ucl.ac.uk Depamen of Mahemaics Univesiy College London 202 The shoes pah beween wo uhs in he eal domain passes hough he complex domain. J. Hadamad Chape The fis fundamenal

More information

A Weighted Moving Average Process for Forecasting. Shou Hsing Shih Chris P. Tsokos

A Weighted Moving Average Process for Forecasting. Shou Hsing Shih Chris P. Tsokos A Weighed Moving Aveage Pocess fo Foecasing Shou Hsing Shih Chis P. Tsokos Depamen of Mahemaics and Saisics Univesiy of Souh Floida, USA Absac The objec of he pesen sudy is o popose a foecasing model fo

More information

Tutorial on Strehl ratio, wavefront power series expansion, Zernike polynomials expansion in small aberrated optical systems By Sheng Yuan

Tutorial on Strehl ratio, wavefront power series expansion, Zernike polynomials expansion in small aberrated optical systems By Sheng Yuan Tutoial on Stel atio, wavefont powe seies expansion, Zenike polynomials expansion in small abeated optical systems By Seng Yuan. Stel Ratio Te wave abeation function, (x,y, is defined as te distance, in

More information

Research on the Algorithm of Evaluating and Analyzing Stationary Operational Availability Based on Mission Requirement

Research on the Algorithm of Evaluating and Analyzing Stationary Operational Availability Based on Mission Requirement Reseach on he Algoihm of Evaluaing and Analyzing Saionay Opeaional Availabiliy Based on ission Requiemen Wang Naichao, Jia Zhiyu, Wang Yan, ao Yilan, Depamen of Sysem Engineeing of Engineeing Technology,

More information

EVENT HORIZONS IN COSMOLOGY

EVENT HORIZONS IN COSMOLOGY Mahemaics Today Vol7(Dec-)54-6 ISSN 976-38 EVENT HORIZONS IN COSMOLOGY K Punachanda Rao Depamen of Mahemaics Chiala Engineeing College Chiala 53 57 Andha Padesh, INDIA E-mail: dkpaocecc@yahoocoin ABSTRACT

More information

Structural Dynamics and Earthquake Engineering

Structural Dynamics and Earthquake Engineering Srucural Dynamics and Earhquae Engineering Course 1 Inroducion. Single degree of freedom sysems: Equaions of moion, problem saemen, soluion mehods. Course noes are available for download a hp://www.c.up.ro/users/aurelsraan/

More information

Reinforcement learning

Reinforcement learning Lecue 3 Reinfocemen leaning Milos Hauskech milos@cs.pi.edu 539 Senno Squae Reinfocemen leaning We wan o lean he conol policy: : X A We see examples of x (bu oupus a ae no given) Insead of a we ge a feedback

More information

PRESSURE DRAWDOWN EQUATIONS FOR MULTIPLE-WELL SYSTEMS IN CIRCULAR-CYLINDRICAL RESERVOIRS

PRESSURE DRAWDOWN EQUATIONS FOR MULTIPLE-WELL SYSTEMS IN CIRCULAR-CYLINDRICAL RESERVOIRS VOL. 8, NO. 7, JULY 013 ISSN 1819-6608 ARPN Jounal of Engineeing and Applied Sciences 006-013 Asian Reseac Publising Netwok (ARPN). All igts eseved. www.apnjounals.com PRESSURE RAWOWN EQUATIONS FOR MULTIPLE-WELL

More information

û s L u t 0 s a ; i.e., û s 0

û s L u t 0 s a ; i.e., û s 0 Te Hille-Yosida Teorem We ave seen a wen e absrac IVP is uniquely solvable en e soluion operaor defines a semigroup of bounded operaors. We ave no ye discussed e condiions under wic e IVP is uniquely solvable.

More information

IMPROVED DESIGN EQUATIONS FOR ASYMMETRIC COPLANAR STRIP FOLDED DIPOLES ON A DIELECTRIC SLAB

IMPROVED DESIGN EQUATIONS FOR ASYMMETRIC COPLANAR STRIP FOLDED DIPOLES ON A DIELECTRIC SLAB IMPROVED DESIGN EQUATIONS FOR ASYMMETRIC COPLANAR STRIP FOLDED DIPOLES ON A DIELECTRIC SLAB H.J. Visse* * Hols Cene TNO P.O. Bo 855 565 N Eindhoven, The Nehelands E-mail: hui.j.visse@no.nl eywods: Coupled

More information

The Quantum Theory of Atoms and Molecules: The Schrodinger equation. Hilary Term 2008 Dr Grant Ritchie

The Quantum Theory of Atoms and Molecules: The Schrodinger equation. Hilary Term 2008 Dr Grant Ritchie e Quanum eory of Aoms and Molecules: e Scrodinger equaion Hilary erm 008 Dr Gran Ricie An equaion for maer waves? De Broglie posulaed a every paricles as an associaed wave of waveleng: / p Wave naure of

More information

Comprehensive Code Verification Techniques for Finite Volume CFD Codes

Comprehensive Code Verification Techniques for Finite Volume CFD Codes Compues and Fluids, 0 Compeensive Code Veificaion Tecniques fo Finie Volume CFD Codes Subamanya P. Velui and Cisope J. Roy Aeospace and Ocean Engineeing Depamen Viginia Tec, Blacksbug, Viginia 406 Edwad

More information

Extremal problems for t-partite and t-colorable hypergraphs

Extremal problems for t-partite and t-colorable hypergraphs Exemal poblems fo -paie and -coloable hypegaphs Dhuv Mubayi John Talbo June, 007 Absac Fix ineges and an -unifom hypegaph F. We pove ha he maximum numbe of edges in a -paie -unifom hypegaph on n veices

More information

Discretization of Fractional Order Differentiator and Integrator with Different Fractional Orders

Discretization of Fractional Order Differentiator and Integrator with Different Fractional Orders Inelligen Conol and Auomaion, 207, 8, 75-85 hp://www.scip.og/jounal/ica ISSN Online: 253-066 ISSN Pin: 253-0653 Disceizaion of Facional Ode Diffeeniao and Inegao wih Diffeen Facional Odes Qi Zhang, Baoye

More information

Department of Chemical Engineering University of Tennessee Prof. David Keffer. Course Lecture Notes SIXTEEN

Department of Chemical Engineering University of Tennessee Prof. David Keffer. Course Lecture Notes SIXTEEN D. Keffe - ChE 40: Hea Tansfe and Fluid Flow Deamen of Chemical Enee Uniesi of Tennessee Pof. Daid Keffe Couse Lecue Noes SIXTEEN SECTION.6 DIFFERENTIL EQUTIONS OF CONTINUITY SECTION.7 DIFFERENTIL EQUTIONS

More information

[ ] 0. = (2) = a q dimensional vector of observable instrumental variables that are in the information set m constituents of u

[ ] 0. = (2) = a q dimensional vector of observable instrumental variables that are in the information set m constituents of u Genealized Mehods of Momens he genealized mehod momens (GMM) appoach of Hansen (98) can be hough of a geneal pocedue fo esing economics and financial models. he GMM is especially appopiae fo models ha

More information

Damage Assessment in Composites using Fiber Bragg Grating Sensors. Mohanraj Prabhugoud

Damage Assessment in Composites using Fiber Bragg Grating Sensors. Mohanraj Prabhugoud ABSTRACT PRABHUGOUD MOHANRAJ. Damage Assessmen in Composies using Fibe Bagg Gaing Sensos. (Unde he diecion of Assisan Pofesso Kaa J. Pees). This disseaion develops a mehodology o assess damage in composies

More information

( ) c(d p ) = 0 c(d p ) < c(d p ) 0. H y(d p )

( ) c(d p ) = 0 c(d p ) < c(d p ) 0. H y(d p ) 8.7 Gavimeic Seling in a Room Conside a oom of volume V, heigh, and hoizonal coss-secional aea A as shown in Figue 8.18, which illusaes boh models. c(d ) = 0 c(d ) < c(d ) 0 y(d ) (a) c(d ) = c(d ) 0 (b)

More information

Non-sinusoidal Signal Generators

Non-sinusoidal Signal Generators Non-sinusoidal Signal Geneaos ecangle, iangle, saw ooh, pulse, ec. Muliibao cicuis: asable no sable saes (wo quasi-sable saes; i emains in each sae fo pedeemined imes) monosable one sable sae, one unsable

More information

Finite-Sample Effects on the Standardized Returns of the Tokyo Stock Exchange

Finite-Sample Effects on the Standardized Returns of the Tokyo Stock Exchange Available online a www.sciencediec.com Pocedia - Social and Behavioal Sciences 65 ( 01 ) 968 973 Inenaional Congess on Inedisciplinay Business and Social Science 01 (ICIBSoS 01) Finie-Sample Effecs on

More information

r r r r r EE334 Electromagnetic Theory I Todd Kaiser

r r r r r EE334 Electromagnetic Theory I Todd Kaiser 334 lecoagneic Theoy I Todd Kaise Maxwell s quaions: Maxwell s equaions wee developed on expeienal evidence and have been found o goven all classical elecoagneic phenoena. They can be wien in diffeenial

More information

Lecture 5. Chapter 3. Electromagnetic Theory, Photons, and Light

Lecture 5. Chapter 3. Electromagnetic Theory, Photons, and Light Lecue 5 Chape 3 lecomagneic Theo, Phoons, and Ligh Gauss s Gauss s Faada s Ampèe- Mawell s + Loen foce: S C ds ds S C F dl dl q Mawell equaions d d qv A q A J ds ds In mae fields ae defined hough ineacion

More information

Risk tolerance and optimal portfolio choice

Risk tolerance and optimal portfolio choice Risk oleance and opimal pofolio choice Maek Musiela BNP Paibas London Copoae and Invesmen Join wok wih T. Zaiphopoulou (UT usin) Invesmens and fowad uiliies Pepin 6 Backwad and fowad dynamic uiliies and

More information

Turbulent buoyant confined jet with variable source temperature

Turbulent buoyant confined jet with variable source temperature Tubulen buoyan confined je wih vaiable souce empeaue M. F. El-Amin 1,, Amgad Salama 1 and Shuyu Sun 1 1 King Abdullah Univesiy of Science and Technology (KAUST), Thuwal 3955-6900, Kingdom of Saudi Aabia

More information

( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba

( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba THE INTEACTION OF ADIATION AND MATTE: SEMICLASSICAL THEOY PAGE 26 III. EVIEW OF BASIC QUANTUM MECHANICS : TWO -LEVEL QUANTUM SYSTEMS : The lieaue of quanum opics and lase specoscop abounds wih discussions

More information

Propagation of Torsional Surface Waves. in Heterogeneous Half-Space. with Irregular Free Surface

Propagation of Torsional Surface Waves. in Heterogeneous Half-Space. with Irregular Free Surface Applied Mahemaical Sciences Vol. 7 no. 9 49 437 Popagaion of Tosional Sface Waves in Heeogeneos Half-Space wih Iegla Fee Sface M. M. Selim Depamen of Mahemaics Facly of Еdcaion Se Canal Univesiy Se Egyp

More information

Problem Set 5: Universal Law of Gravitation; Circular Planetary Orbits

Problem Set 5: Universal Law of Gravitation; Circular Planetary Orbits Poblem Set 5: Univesal Law of Gavitation; Cicula Planetay Obits Design Engineeing Callenge: Te Big Dig.007 Contest Evaluation of Scoing Concepts: Spinne vs. Plowe PROMBLEM 1: Daw a fee-body-diagam of a

More information

The Method of Images in Velocity-Dependent Systems

The Method of Images in Velocity-Dependent Systems >1< The Mehod of Images in Velociy-Dependen Sysems Dan Censo Ben Guion Univesiy of he Negev Depamen of Elecical and Compue Engineeing Bee Sheva, Isael 8415 censo@ee.bgu.ac.il Absac This sudy invesigaes

More information