University of Pisa. N. Zaccari, D. Aquaro. Pebble Beds. - ITALY - Department of Mechanical, Nuclear and Production Engineering

Size: px
Start display at page:

Download "University of Pisa. N. Zaccari, D. Aquaro. Pebble Beds. - ITALY - Department of Mechanical, Nuclear and Production Engineering"

Transcription

1 Univesity f Pisa - ITALY - Depatment f Mechanical, Nuclea and Pductin Engineeing Them-Mechanical Behaviu f Li 4 SO 4 and Li TiO 3 N. Zaccai, D. Aqua

2 Cntents f Pesentatin This pesentatin descibes the them-mechanical test n ceamics Pebble bed mateials candidate as ceamic beede mateials in a Fusin eacts Li 4 SiO 4 φ mm Ppeties Li TiO 3 Li 4 SiO 4 Li TiO 3 φ.8 - mm Density (g/cm 3 ) Psity % E yung (GPa) Ceff. Pissn ν Stenght Raptue (MPa) Yielding stess (MPa) Cnductiv ity (W/mK) at 98 K This eseach aims t veify the pssibility f simulate the them-mechanical behaviu f this mateials with a theetical mdel develped by the auths Them-Mechanical Behaviu f

3 Cntents f Pesentatin Desciptin f a epeimental set-up t investigate the Them-mechanical behavi f pebble bed Desciptin f a new instumentatin t measue the lcal packing fact f pebble bed Desciptin f the theetical mdel Results f the epeiments and cmpaisn with the theetical mdel Cnclusin Them-Mechanical Behaviu f 3

4 Epeimental Set-up Hydaulic pistn Unaial defmatin test Cnductivity test vesus aial defmatin with and withut gas Lad Cell Tns N. Zaccai, D. Aqua Epeimental and numeical analysis n Pebble beds used in an ITER Test Mdule Blanket, ISFTN-7, Tky, Japan, May -6, 5 Them-Mechanical Behaviu f 4

5 Epeimental Set-up Cppe plate Themcuples Cylinde that cntain the pebble bed Guaded Themal Resistance Cental Themal Resistance Them-Mechanical Behaviu f Blanket Themal Resistance 5

6 Epeimental Equipment Themcuples Gas Cnduct Them-Mechanical Behaviu f 6

7 Epeimental Equipment Filling f cylinde that cntains the bed Bed vib-cmpactin The themal cnductivity f Pebble-bed is detemined by cmpaisn with a efeence mateial (in this test alumina ALUBIT 9) LabView Cntl Panel ) The lad was inceased deceased step by step. ) Each lading step was held f the time inteval needed t each a steady state heat tansfe cnditin, in de t detemine the themal cnductivity vesus aial defmatin. TEST CONDITION: - Packing fact.635 f Li TiO 3 and.68 f Li 4 SiO 4 -ma Pessue 6.6 MPa -Aveage temp. In the bed 3 K -Ai atm and vacuum 6.5e-3 atm Them-Mechanical Behaviu f 7

8 Peliminay gamma ay densimete This device is made up f : ) a lead cylinde ) the scintillat detect (Na I) 3) the gamma suce The lead cylinde is put in psitin n the pebble bed by means f a cicula plate (with a buttnhle) cnnected t the cntaine f the pebble bed Them-Mechanical Behaviu f 8

9 Peliminay gamma ay densimete T measue the density f mateial, we take in accunt nly the gamma backscatte peak (.8,4 Mev) This instumentatin supply, in the field pints, the aveage density f pebble bed thickness Calibatin cuve Field pints Them-Mechanical Behaviu f 9

10 Theetical elastic-plastic D mdel f a tw half sphees Theetical Mdel f them-mechanical mechanical behaviu f pebble bed stiffness cnductivity Etensin t 3D mdel Simple lattices cmpsed f sphees The develped mdel has been cmpaed with the epeimental esults btained by eseach n the slid beeding blanket f Fusin Nuclea React. [] D. Aqua, Themal Mechanical Analysis f a Slid Beeding Blanket, Fusin Eng. Des., 69 (3) [] D. Aqua, N. Zaccai, Mitigatin f a Ce Meltdwn Scenai by Means f a Ce Catche Lcated Inside The React Pessue Vessel, th ICONE, Alingtn, Viginia (Washingtn, D.C.), USA, Apil 5-9, 4. [3] D. Aqua, N. Zaccai, Themal Analysis f a Ce Catche Made f Pebble Bed Lcated Inside The React Pessue Vessel, Int. Junal f Heat and Technlgy, vl., Januay 5, -9. [4] D. Aqua, N. Zaccai, Pebble Bed Themal-Mechanical Theetical Mdel: Applicatin at The Gemety f Test Blanket Mdule f ITER-FEAT Nuclea Fusin React, Fusin Engineeing and Design, in pess, 5. Them-Mechanical Behaviu f

11 Them-Mechanical Behaviu f Theetical Mdel Theetical Mdel Effective stiffness f tw half sphee Effective stiffness f tw half sphee σ σ E E σ σ ε E u / / ln σ 3.5 E P y e σ X p (MPa); q (W/m ) Effective stiffness ( ) E P u P K / ) / ) /( / ( ln ) ( / σ E E P u P K y p σ σ ε ln ) ( Elastic egimen Plastic egimen Sphee stess tend (ο) ο σ σy ο The main hyptheses f the them-mechanical theetical mdel ae the fllwing: the mateial behaviu is elastic-pefectly plastic the sphee is cnsideed a mn dimensinal beam with a vaiable css-sectin the mateial cnductivity is cnstant with the tempeatue

12 Them-Mechanical Behaviu f Theetical Mdel Theetical Mdel Effective cnductivity f tw half sphees cmpessed by a fce Effective cnductivity f tw half sphees cmpessed by a fce P in elastic P in elastic-plastic egimen plastic egimen T dv q V H V eq Δ & λ The effective cnductivity f tw half sphees cmpessed by a fce P, can be given by the fllwing fmula: X p (MPa); q (W/m ) sf sf c c eq eq R V V R V V R * * λ The ttal themal esistance is btained by additining f the sphee themal esistance and the cntact themal esistance P E R eq λ ν λ π ln 3 ) 9 ( R eq λ λ ln Themal esistance f tw half sphee Elastic egimen Plastic egimen The plastic zne is simulated by a cylinde that it have the same vlume f a the plastic sphee sect

13 Theetical Mdel Effective stiffness and cnductibility f cubic simple lattice We cnsideed the bed made f egula lattices which ae chaacteized by diffeent values f packing fact γ, in paticula : simple cubic lattice: γ.536; bdy cented cubic lattice : γ.68; face cented cubic lattice : γ.74 λ CS π R 3R CS S eq λ CC.94 π R.987 CC S Req λ FC.88 π R.486 R FC S eq K R Z 8 K K K csα. 44 K 4 R R SS KY K X 4 Keq Keq Z X Y SS K K Y K K 4( K ). 47 K X Z Y eq Them-Mechanical Behaviu f 3

14 Theetical Mdel Cack Ppagatin In de t simulate the cacking and cushing effect f ceamics mateials, we have cnsideed that the adius f sphees decease when the cmpessin lad incease because a pat f mateial (afte the cacking) desn t cntibute t the mechanical esistance. The plastic mateial is simulated like a fluid which pduces a tensile stess nmally t the applied lad. This tensile can cack the sphee mateial. Vn Mises Stess (ma MPa) Analisi tem-meccanica di letti di sfee D.Aqua, N. Zaccai, 5 R.L. n 78 DIMNP Univ. Di Pisa- Italy. Radial cack ppagatin aund the cntact zne Them-Mechanical Behaviu f 4

15 Results Li TiO 3 Pessue vesus aial defmatin cuve Cuve f themal cnductivity vesus pessue Pessue (MPa) defmatin, ε % Cnductivity (W/mK) Pessue (MPa) ai atm at T3K vacuum 6.5e-3 atm at 3K I Cycle Ma Pessue: 6.6 MPa Ma defmatin:.73 % II Cycle Ma Pessue: 6.5 MPa Ma defmatin:.9 % Ma cnductivity (ai):.38 W/mK Min cnductivity (ai):.6 W/mK Ma cnductivity (vacuum):.3 W/mK Ma cnductivity (vacuum):.9 W/mK Them-Mechanical Behaviu f 5

16 Distibutin paametes Packing fact Aveage Befe the test γ.63 Results Li TiO 3 Befe the test 5 Radial distibutin f the packing fact 5 Afte the test 6 Afte the test γ. 64 Pecentage f the pebble bed vlume which has a paticula value f packing fact % in vlume Befe the test Afte the test ange f Packing Fact Them-Mechanical Behaviu f 6

17 Results Li 4 SiO 4 Pessue vesus aial defmatin cuve Cuve f themal cnductivity vesus pessue Pessue (MPa) defmatin ε % Cnductivity (W/mK) ai atm at T3K vacuum 6.5e-3 atm at T3K Pessue (MPa) I Cycle Ma Pessue: 6.45 MPa Ma defmatin:.55 % II Cycle Ma Pessue: 6.6 MPa Ma defmatin:.83 % Ma cnductivity (ai):.3 W/mK Min cnductivity (ai):.4 W/mK Ma cnductivity (vacuum):.6 W/mK Ma cnductivity (vacuum):. W/mK Them-Mechanical Behaviu f 7

18 Distibutin paametes Packing fact Aveage Befe the test γ.65 Results Li 4 SiO 4 Radial distibutin f the packing fact Befe the test Afte the test.65 Afte the test γ Pecentage f the pebble bed vlume which has a paticula value f packing fact % in vlum e Befe the test Afte the test Range f Packing Fact Them-Mechanical Behaviu f 8

19 S.E.M. pht n cacked Pebble bed Cntact zne Cushed sphees Them-Mechanical Behaviu f 9

20 S.E.M. pht n cacked Pebble bed Seveal pebbles agglmeated themselves abve all in the cental pat f the bed. The cntact aea lks like a cylinde cacked The cacks ae due t tensile esidual stesses which develp duing the unlading. The mateial f the cntact cylinde was analysed and it pved have the same cmpsitin f the pebble mateial. Them-Mechanical Behaviu f

21 Pessue (MPa) Results Cmpaisn between Theetical mdel and Epeimental esults Li 4 SiO 4 φ mm Li TiO 3 φ.8 - mm Theetical Epeimental ( cycle) Defmatin ε (%) Pessue (Mpa) Theetical Epeimental ( cycle).5.5 Defmatin ε (%).7.6 Cnductivity (W/mK) Epeimental, mean T3K Theetical Cnductivity (W/mK) Epeimental (mean T3 K) Theetical Pessue (MPa) Them-Mechanical Behaviu f Pessue (MPa)

22 FUTURE DEVELOPMENT Discete Mdel f Pebble bed Them-Mechanical Behaviu f

23 CONCLUSION The tests have pemitted t detemine the effective stiffness and cnductivity f the pebble beds vesus aial defmatin; The adial distibutin f the packing fact has been detemined by means f a peliminay gamma ay device. We can pint ut that bed cmpessin pduces a me unifm distibutin f the packing fact. The cmpaisn with the theetical mdel shws a gd ageement f the epeimental effective cnductivity and stiffness f the bed abve all in the elasticplastic defmatin; Develpment f the mdel ae being pefmed in de t simulate the aangement phase. Them-Mechanical Behaviu f 3

Journal of Solid Mechanics and Materials Engineering

Journal of Solid Mechanics and Materials Engineering Junal f Slid Mechanics and Mateials Engineeing Vl. 4, N. 8, 21 Themal Stess and Heat Tansfe Cefficient f Ceamics Stalk Having Ptubeance Dipping int Mlten Metal* Na-ki NOD**, Henda**, Wenbin LI**, Yasushi

More information

CHAPTER 24 GAUSS LAW

CHAPTER 24 GAUSS LAW CHAPTR 4 GAUSS LAW LCTRIC FLUX lectic flux is a measue f the numbe f electic filed lines penetating sme suface in a diectin pependicula t that suface. Φ = A = A csθ with θ is the angle between the and

More information

Outline. Steady Heat Transfer with Conduction and Convection. Review Steady, 1-D, Review Heat Generation. Review Heat Generation II

Outline. Steady Heat Transfer with Conduction and Convection. Review Steady, 1-D, Review Heat Generation. Review Heat Generation II Steady Heat ansfe ebuay, 7 Steady Heat ansfe wit Cnductin and Cnvectin ay Caett Mecanical Engineeing 375 Heat ansfe ebuay, 7 Outline eview last lectue Equivalent cicuit analyses eview basic cncept pplicatin

More information

5/20/2011. HITT An electron moves from point i to point f, in the direction of a uniform electric field. During this displacement:

5/20/2011. HITT An electron moves from point i to point f, in the direction of a uniform electric field. During this displacement: 5/0/011 Chapte 5 In the last lectue: CapacitanceII we calculated the capacitance C f a system f tw islated cnducts. We als calculated the capacitance f sme simple gemeties. In this chapte we will cve the

More information

Application of Net Radiation Transfer Method for Optimization and Calculation of Reduction Heat Transfer, Using Spherical Radiation Shields

Application of Net Radiation Transfer Method for Optimization and Calculation of Reduction Heat Transfer, Using Spherical Radiation Shields Wld Applied Sciences Junal (4: 457-46, 00 ISSN 88-495 IDOSI Publicatins, 00 Applicatin f Net Radiatin Tansfe Methd f Optimizatin and Calculatin f Reductin Heat Tansfe, Using Spheical Radiatin Shields Seyflah

More information

CHAPTER GAUSS'S LAW

CHAPTER GAUSS'S LAW lutins--ch 14 (Gauss's Law CHAPTE 14 -- GAU' LAW 141 This pblem is ticky An electic field line that flws int, then ut f the cap (see Figue I pduces a negative flux when enteing and an equal psitive flux

More information

Example

Example hapte Exaple.6-3. ---------------------------------------------------------------------------------- 5 A single hllw fibe is placed within a vey lage glass tube. he hllw fibe is 0 c in length and has a

More information

A) (0.46 î ) N B) (0.17 î ) N

A) (0.46 î ) N B) (0.17 î ) N Phys10 Secnd Maj-14 Ze Vesin Cdinat: xyz Thusday, Apil 3, 015 Page: 1 Q1. Thee chages, 1 = =.0 μc and Q = 4.0 μc, ae fixed in thei places as shwn in Figue 1. Find the net electstatic fce n Q due t 1 and.

More information

A Direct Method for the Evaluation of Lower and Upper Bound Ratchet Limits

A Direct Method for the Evaluation of Lower and Upper Bound Ratchet Limits A Diect Methd f the Evaluatin f Lwe and Uppe Bund Ratchet Limits J. Ue a, H. Chen a, T. Li a, W. Chen a, D. Tipping b, D. Macenzie a a Dept f Mechanical Engineeing, Univesity f Stathclyde, Glasgw, Sctland,

More information

Electric Charge. Electric charge is quantized. Electric charge is conserved

Electric Charge. Electric charge is quantized. Electric charge is conserved lectstatics lectic Chage lectic chage is uantized Chage cmes in incements f the elementay chage e = ne, whee n is an intege, and e =.6 x 0-9 C lectic chage is cnseved Chage (electns) can be mved fm ne

More information

A) 100 K B) 150 K C) 200 K D) 250 K E) 350 K

A) 100 K B) 150 K C) 200 K D) 250 K E) 350 K Phys10 Secnd Maj-09 Ze Vesin Cdinat: k Wednesday, May 05, 010 Page: 1 Q1. A ht bject and a cld bject ae placed in themal cntact and the cmbinatin is islated. They tansfe enegy until they each a final equilibium

More information

Journal of Theoretics

Journal of Theoretics Junal f Theetics Junal Hme Page The Classical Pblem f a Bdy Falling in a Tube Thugh the Cente f the Eath in the Dynamic They f Gavity Iannis Iaklis Haanas Yk Univesity Depatment f Physics and Astnmy A

More information

ME 3600 Control Systems Frequency Domain Analysis

ME 3600 Control Systems Frequency Domain Analysis ME 3600 Cntl Systems Fequency Dmain Analysis The fequency espnse f a system is defined as the steady-state espnse f the system t a sinusidal (hamnic) input. F linea systems, the esulting utput is itself

More information

Clean Technol., Vol. 22, No. 1, March 2016, pp

Clean Technol., Vol. 22, No. 1, March 2016, pp lean echnl., Vl., N. 1, Mach 016, pp. 45-5 청정에너지기술 mpaisn between Wate and N-etadecane as Insulatin Mateials thugh Mdeling and Simulatin f Heat ansfe in Pacaging Bx f Vaccine Shipping Van-Dung Da 1, I-Kyu

More information

EFFECT OF VARIATION IN LENGTH OF THE CONVENTIONAL HEAT PIPE ON THE THERMAL PERFORMANCE

EFFECT OF VARIATION IN LENGTH OF THE CONVENTIONAL HEAT PIPE ON THE THERMAL PERFORMANCE EFFECT OF VAIATION IN LENGTH OF THE CONVENTIONAL HEAT PIPE ON THE THEMAL PEFOMANCE Yung Min Se, Yng Gap Pak and Man Yeng Ha* *Auth f cespndence Schl f Mechanical Engineeing, Pusan Natinal Uniesity, Suth

More information

A Direct Method for the Evaluation of Lower and Upper Bound Ratchet Limits

A Direct Method for the Evaluation of Lower and Upper Bound Ratchet Limits Ue, James Michael and Chen, Hafeng and Chen, Weihang and Li, Tianbai and Tipping, James and Macenzie, Dnald (211) A diect methd f the evaluatin f lwe and uppe bund atchet limits. In: 11th Intenatinal Cnfeence

More information

Strees Analysis in Elastic Half Space Due To a Thermoelastic Strain

Strees Analysis in Elastic Half Space Due To a Thermoelastic Strain IOSR Junal f Mathematics (IOSRJM) ISSN: 78-578 Vlume, Issue (July-Aug 0), PP 46-54 Stees Analysis in Elastic Half Space Due T a Themelastic Stain Aya Ahmad Depatment f Mathematics NIT Patna Biha India

More information

A) N B) 0.0 N C) N D) N E) N

A) N B) 0.0 N C) N D) N E) N Cdinat: H Bahluli Sunday, Nvembe, 015 Page: 1 Q1. Five identical pint chages each with chage =10 nc ae lcated at the cnes f a egula hexagn, as shwn in Figue 1. Find the magnitude f the net electic fce

More information

Introduction. Electrostatics

Introduction. Electrostatics UNIVESITY OF TECHNOLOGY, SYDNEY FACULTY OF ENGINEEING 4853 Electmechanical Systems Electstatics Tpics t cve:. Culmb's Law 5. Mateial Ppeties. Electic Field Stength 6. Gauss' Theem 3. Electic Ptential 7.

More information

Magnetism. Chapter 21

Magnetism. Chapter 21 1.1 Magnetic Fields Chapte 1 Magnetism The needle f a cmpass is pemanent magnet that has a nth magnetic ple (N) at ne end and a suth magnetic ple (S) at the the. 1.1 Magnetic Fields 1.1 Magnetic Fields

More information

Sensors and Actuators Introduction to sensors

Sensors and Actuators Introduction to sensors Senss and Actuats Intductin t senss Sande Stuij (s.stuij@tue.nl) Depatment f Electical Engineeing Electnic Systems AMPLIFIES (Chapte 5.) Infmatin pcessing system nncntact sens cntact sens abslute sens

More information

CHE CHAPTER 11 Spring 2005 GENERAL 2ND ORDER REACTION IN TURBULENT TUBULAR REACTORS

CHE CHAPTER 11 Spring 2005 GENERAL 2ND ORDER REACTION IN TURBULENT TUBULAR REACTORS CHE 52 - CHPTE Sping 2005 GENEL 2ND ODE ECTION IN TUULENT TUUL ECTOS Vassilats & T, IChEJ. (4), 666 (965) Cnside the fllwing stichiety: a + b = P The ass cnsevatin law f species i yields Ci + vci =. Di

More information

Steady State Analysis of Squirrel-Cage Induction Machine with Skin-Effect

Steady State Analysis of Squirrel-Cage Induction Machine with Skin-Effect Steady State Analysis f Squiel-Cage Inductin Machine with Skin-Effect D.-Ing. O. I. Ok Depatment f Electical Engineeing Univesity f Nigeia, Nsukka Enugu State, Nigeia. Email: gnnayak@htmail.cm ABSTACT

More information

Example 11: The man shown in Figure (a) pulls on the cord with a force of 70

Example 11: The man shown in Figure (a) pulls on the cord with a force of 70 Chapte Tw ce System 35.4 α α 100 Rx cs 0.354 R 69.3 35.4 β β 100 Ry cs 0.354 R 111 Example 11: The man shwn in igue (a) pulls n the cd with a fce f 70 lb. Repesent this fce actin n the suppt A as Catesian

More information

FE FORMULATIONS FOR PLASTICITY

FE FORMULATIONS FOR PLASTICITY G These slides ae designed based on the book: Finite Elements in Plasticity Theoy and Pactice, D.R.J. Owen and E. Hinton, 970, Pineidge Pess Ltd., Swansea, UK. Couse Content: A INTRODUCTION AND OVERVIEW

More information

Subjects discussed: Aircraft Engine Noise : Principles; Regulations

Subjects discussed: Aircraft Engine Noise : Principles; Regulations 16.50 Lectue 36 Subjects discussed: Aicaft Engine Nise : Pinciples; Regulatins Nise geneatin in the neighbhds f busy aipts has been a seius pblem since the advent f the jet-pweed tanspt, in the late 1950's.

More information

OBJECTIVE To investigate the parallel connection of R, L, and C. 1 Electricity & Electronics Constructor EEC470

OBJECTIVE To investigate the parallel connection of R, L, and C. 1 Electricity & Electronics Constructor EEC470 Assignment 7 Paallel Resnance OBJECTIVE T investigate the paallel cnnectin f R,, and C. EQUIPMENT REQUIRED Qty Appaatus 1 Electicity & Electnics Cnstuct EEC470 1 Basic Electicity and Electnics Kit EEC471-1

More information

On the structure of MHD shock waves in a viscous gas

On the structure of MHD shock waves in a viscous gas On the stuctue f MHD shck waves in a viscus gas On the stuctue f MHD shck waves in a viscus gas R. K. Anand and Haish C. Yadav Depatment f Physics, Univesity f Allahabad, Allahabad-, India e-mail: anand.ajkuma@ediffmail.cm

More information

The Gradient and Applications This unit is based on Sections 9.5 and 9.6, Chapter 9. All assigned readings and exercises are from the textbook

The Gradient and Applications This unit is based on Sections 9.5 and 9.6, Chapter 9. All assigned readings and exercises are from the textbook The Gadient and Applicatins This unit is based n Sectins 9.5 and 9.6 Chapte 9. All assigned eadings and eecises ae fm the tetbk Objectives: Make cetain that u can define and use in cntet the tems cncepts

More information

Physics 111. Exam #1. January 26, 2018

Physics 111. Exam #1. January 26, 2018 Physics xam # Januay 6, 08 ame Please ead and fllw these instuctins caefully: Read all pblems caefully befe attempting t slve them. Yu wk must be legible, and the ganizatin clea. Yu must shw all wk, including

More information

Electromagnetic Waves

Electromagnetic Waves Chapte 3 lectmagnetic Waves 3.1 Maxwell s quatins and ectmagnetic Waves A. Gauss s Law: # clsed suface aea " da Q enc lectic fields may be geneated by electic chages. lectic field lines stat at psitive

More information

Surface and Interface Science Physics 627; Chemistry 542. Lecture 10 March 1, 2013

Surface and Interface Science Physics 627; Chemistry 542. Lecture 10 March 1, 2013 Suface and Inteface Science Physics 67; Chemisty 54 Lectue 0 Mach, 03 Int t Electnic Ppeties: Wk Functin,Theminic Electn Emissin, Field Emissin Refeences: ) Wduff & Delcha, Pp. 40-4; 46-484 ) Zangwill

More information

Announcements Candidates Visiting Next Monday 11 12:20 Class 4pm Research Talk Opportunity to learn a little about what physicists do

Announcements Candidates Visiting Next Monday 11 12:20 Class 4pm Research Talk Opportunity to learn a little about what physicists do Wed., /11 Thus., /1 Fi., /13 Mn., /16 Tues., /17 Wed., /18 Thus., /19 Fi., / 17.7-9 Magnetic Field F Distibutins Lab 5: Bit-Savat B fields f mving chages (n quiz) 17.1-11 Pemanent Magnets 18.1-3 Mic. View

More information

MEM202 Engineering Mechanics Statics Course Web site:

MEM202 Engineering Mechanics Statics Course Web site: 0 Engineeing Mechanics - Statics 0 Engineeing Mechanics Statics Cuse Web site: www.pages.dexel.edu/~cac54 COUSE DESCIPTION This cuse cves intemediate static mechanics, an extensin f the fundamental cncepts

More information

Solutions: Solution. d = 3.0g/cm we can calculate the number of Xe atoms per unit volume, Given m and the given values from Table 7.

Solutions: Solution. d = 3.0g/cm we can calculate the number of Xe atoms per unit volume, Given m and the given values from Table 7. Tutial-09 Tutial - 09 Sectin6: Dielectic Mateials ECE:09 (Electnic and Electical Ppeties f Mateials) Electical and Cmpute Engineeing Depatment Univesity f Watel Tut: Hamid Slutins: 7.3 Electnic plaizatin

More information

SOURCE MODEL OF THE 2010 ELAZIG KOVANCILAR EARTHQUAKE (M w 6.1) FOR BROADBAND GROUND MOTION SIMULATION

SOURCE MODEL OF THE 2010 ELAZIG KOVANCILAR EARTHQUAKE (M w 6.1) FOR BROADBAND GROUND MOTION SIMULATION SOURCE MODEL OF THE 200 ELAZIG KOVANCILAR EARTHQUAKE (M w 6.) FOR BROADBAND GROUND MOTION SIMULATION Mehmet Baykal MEE0509 Supevis: Hie Miyake ABSTRACT On 8 Mach 200, an eathquake f M w =6. ccued in Elazig

More information

Problem 1: Multiple Choice Questions

Problem 1: Multiple Choice Questions Mathematics 102 Review Questions Poblem 1: Multiple Choice Questions 1: Conside the function y = f(x) = 3e 2x 5e 4x (a) The function has a local maximum at x = (1/2)ln(10/3) (b) The function has a local

More information

COMPARISON OF METHODS FOR SOLVING THE HEAT TRANSFER IN ELECTRICAL MACHINES

COMPARISON OF METHODS FOR SOLVING THE HEAT TRANSFER IN ELECTRICAL MACHINES POZNAN UNIVE RSITY OF TE CHNOLOGY ACADE MIC JOURNALS No 75 Electical Engineeing 2013 Zbynek MAKKI* Macel JANDA* Ramia DEEB* COMPARISON OF METHODS FOR SOLVING THE HEAT TRANSFER IN ELECTRICAL MACHINES This

More information

Performance Analysis of Household Refrigerator with Alternate Refrigerants

Performance Analysis of Household Refrigerator with Alternate Refrigerants ISSN: 239-873 Intenatinal Junal f Innvative Reseach in Science, Engineeing and Technlgy (An ISO 3297: 2007 Cetified Oganizatin) Vl. 3, Issue 4, Apil 204 Pefmance Analysis f Husehld Refigeat with Altenate

More information

THE SPATIAL CROSS-CORRELATION OF. Mobile and Portable Radio Research Group

THE SPATIAL CROSS-CORRELATION OF. Mobile and Portable Radio Research Group FFCTS OF MULTIPATH AGULAR SPRAD O TH SPATIAL CROSS-CORRLATIO OF RCIVD VOLTAG VLOPS Gegy D. Dugin and Thede S. Rappapt Mbile and Ptable Radi Reseach Gup Badley Depatment f lectical and Cmpute ngineeing

More information

Gelation and Time-Dependent Rheological Behavior of Oil / Synthetic Based Drilling Fluids

Gelation and Time-Dependent Rheological Behavior of Oil / Synthetic Based Drilling Fluids AADE-11-NTCE-81 Gelatin and Time-Dependent Rhelgical Behavi f Oil / Synthetic Based Dilling Fluids Gkem M. Gkdemi, Even M. Ozbaglu, Reza Majidi, Stefan Z. Miska, Nichlas Takach, and Mengjia Yu, The Univesity

More information

3D FE Modeling Simulation of Cold Rotary Forging with Double Symmetry Rolls X. H. Han 1, a, L. Hua 1, b, Y. M. Zhao 1, c

3D FE Modeling Simulation of Cold Rotary Forging with Double Symmetry Rolls X. H. Han 1, a, L. Hua 1, b, Y. M. Zhao 1, c Materials Science Frum Online: 2009-08-31 ISSN: 1662-9752, Vls. 628-629, pp 623-628 di:10.4028/www.scientific.net/msf.628-629.623 2009 Trans Tech Publicatins, Switzerland 3D FE Mdeling Simulatin f Cld

More information

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below.

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below. Fall 2007 Qualifie Pat II 12 minute questions 11) A thin, unifom od of mass M is suppoted by two vetical stings, as shown below. Find the tension in the emaining sting immediately afte one of the stings

More information

Mathematical Models of Dusty Gas Flow through Porous Media

Mathematical Models of Dusty Gas Flow through Porous Media Mathematical Mdels f Dusty Gas Flw thugh Pus Media M.H. HAMDAN Depatment f Mathematical ciences Univesity f New Bunswick P.O. Bx 5050, aint Jhn, New Bunswick, EL 4L5 CANADA hamdan@unb.ca Abstact:- This

More information

EFFECTS OF GFRP REINFORCING REBARS ON SHRINKAGE AND THERMAL STRESSES IN CONCRETE

EFFECTS OF GFRP REINFORCING REBARS ON SHRINKAGE AND THERMAL STRESSES IN CONCRETE EFFECTS OF GFRP REINFORCING REBARS ON SHRINKAGE AND THERMAL STRESSES IN CONCRETE Roge H. L. Chen 1 and Jeong-Hoon Choi 2 ABSTRACT The use of Glass Fibe Reinfoced Polyme (GFRP) ebas instead of conventional

More information

Work, Energy, and Power. AP Physics C

Work, Energy, and Power. AP Physics C k, Eneg, and Pwe AP Phsics C Thee ae man diffeent TYPES f Eneg. Eneg is expessed in JOULES (J) 4.19 J = 1 calie Eneg can be expessed me specificall b using the tem ORK() k = The Scala Dt Pduct between

More information

Today in Astronomy 142: the Milky Way s disk

Today in Astronomy 142: the Milky Way s disk Today in Astonomy 14: the Milky Way s disk Moe on stas as a gas: stella elaxation time, equilibium Diffeential otation of the stas in the disk The local standad of est Rotation cuves and the distibution

More information

CANKAYA UNIVERSITY FACULTY OF ENGINEERING MECHANICAL ENGINEERING DEPARTMENT ME 313 HEAT TRANSFER

CANKAYA UNIVERSITY FACULTY OF ENGINEERING MECHANICAL ENGINEERING DEPARTMENT ME 313 HEAT TRANSFER CANKAYA UNIVERSITY FACUTY OF ENGINEERING MECHANICA ENGINEERING DEPARTMENT ME 313 HEAT TRANSFER CHAPTER-3 EXAMPES 1) Cnsider a slab f thicness as illustrated in figure belw. A fluid at temperature T 1 with

More information

ELECTROMAGNETIC INDUCTION PREVIOUS EAMCET BITS

ELECTROMAGNETIC INDUCTION PREVIOUS EAMCET BITS P P Methd EECTOMAGNETIC INDUCTION PEVIOUS EAMCET BITS [ENGINEEING PAPE]. A cnduct d f length tates with angula speed ω in a unifm magnetic field f inductin B which is pependicula t its mtin. The induced

More information

Chapter 4 Motion in Two and Three Dimensions

Chapter 4 Motion in Two and Three Dimensions Chapte 4 Mtin in Tw and Thee Dimensins In this chapte we will cntinue t stud the mtin f bjects withut the estictin we put in chapte t me aln a staiht line. Instead we will cnside mtin in a plane (tw dimensinal

More information

Lecture #2 : Impedance matching for narrowband block

Lecture #2 : Impedance matching for narrowband block Lectue # : Ipedance atching f nawband blck ichad Chi-Hsi Li Telephne : 817-788-848 (UA) Cellula phne: 13917441363 (C) Eail : chihsili@yah.c.cn 1. Ipedance atching indiffeent f bandwidth ne pat atching

More information

Fri. 10/23 (C14) Linear Dielectrics (read rest at your discretion) Mon. (C 17) , E to B; Lorentz Force Law: fields

Fri. 10/23 (C14) Linear Dielectrics (read rest at your discretion) Mon. (C 17) , E to B; Lorentz Force Law: fields Fi. 0/23 (C4) 4.4. Linea ielectics (ead est at yu discetin) Mn. (C 7) 2..-..2, 2.3. t B; 5..-..2 Lentz Fce Law: fields Wed. and fces Thus. (C 7) 5..3 Lentz Fce Law: cuents Fi. (C 7) 5.2 Bit-Savat Law HW6

More information

10. Groundwater in geotechnical problems

10. Groundwater in geotechnical problems . Goundwate in geotechnical poblems Goundwate plays a key ole in many geotechnical poblems. We will look at; - land subsidence - dewateing open pits - Consolidation of sediments Remembe the stoage of wate

More information

ELASTIC ANALYSIS OF CIRCULAR SANDWICH PLATES WITH FGM FACE-SHEETS

ELASTIC ANALYSIS OF CIRCULAR SANDWICH PLATES WITH FGM FACE-SHEETS THE 9 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS ELASTIC ANALYSIS OF CIRCULAR SANDWICH PLATES WITH FGM FACE-SHEETS R. Sbulati *, S. R. Atashipou Depatment of Civil, Chemical and Envionmental Engineeing,

More information

, and the curve BC is symmetrical. Find also the horizontal force in x-direction on one side of the body. h C

, and the curve BC is symmetrical. Find also the horizontal force in x-direction on one side of the body. h C Umeå Univesitet, Fysik 1 Vitaly Bychkov Pov i teknisk fysik, Fluid Dynamics (Stömningsläa), 2013-05-31, kl 9.00-15.00 jälpmedel: Students may use any book including the textbook Lectues on Fluid Dynamics.

More information

Article : 8 Article : 8 Stress Field. and. Singularity Problem

Article : 8 Article : 8 Stress Field. and. Singularity Problem Aticle : 8 Aticle : 8 Stess Field and Singulaity Poblem (fatigue cack gowth) Repeated load cycles cack development Time (cycles) Cack length 3 Weakening due to gowing cacks Cack length stess concentation

More information

One-Dimensional, Steady-State. State Conduction with Thermal Energy Generation

One-Dimensional, Steady-State. State Conduction with Thermal Energy Generation One-Dimensional, Steady-State State Conduction with Themal Enegy Geneation Implications of Enegy Geneation Involves a local (volumetic) souce of themal enegy due to convesion fom anothe fom of enegy in

More information

Pressure Calculation of a Constant Density Star in the Dynamic Theory of Gravity

Pressure Calculation of a Constant Density Star in the Dynamic Theory of Gravity Pessue Calculation of a Constant Density Sta in the Dynamic Theoy of Gavity Ioannis Iaklis Haanas Depatment of Physics and Astonomy Yok Univesity A Petie Science Building Yok Univesity Toonto Ontaio CANADA

More information

NUMERICAL EVALUATION ON FLOOR COOLING CAPACITY IN AN AIRPORT AH, Nijmegen, the Netherlands Tianjin, China

NUMERICAL EVALUATION ON FLOOR COOLING CAPACITY IN AN AIRPORT AH, Nijmegen, the Netherlands Tianjin, China ceedings: Building Simulatin 07 NUMEICAL EVALUATION ON FLOO COOLING CAACITY IN AN AIOT 3,3, Bing Yu, J.. uchti and.g. Luscuee Divisin Building Sevices, yal Haskning Gup, stbx 5 6500 AH, Nijmegen, the Nethelands

More information

Optimal Design of Transonic Fan Blade Leading Edge Shape Using CFD and Simultaneous Perturbation Stochastic Approximation Method

Optimal Design of Transonic Fan Blade Leading Edge Shape Using CFD and Simultaneous Perturbation Stochastic Approximation Method 1 Optimal Design f Tansnic Fan Blade Leading Edge Shape Using CFD and Simultaneus Petubatin Stchastic Appximatin Methd X.Q.Xing and M.Damdaan Abstact Simultaneus Petubatin Stchastic Appximatin methd has

More information

Methods For High Resistivity Measurements Related To Spacecraft Charging

Methods For High Resistivity Measurements Related To Spacecraft Charging Utah State Univesity DigitalCmmns@USU Junal Aticles Mateials hysics 10-2006 Methds F High Resistivity Measuements Related T Spacecaft Chaging JR Dennisn Utah State Univesity Jeilyn Bunsn Utah State Univesity

More information

STUDY ON 2-D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING

STUDY ON 2-D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING Study Rev. Adv. on -D Mate. shock Sci. wave 33 (13) pessue 111-118 model in mico scale lase shock peening 111 STUDY ON -D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING Y.J. Fan 1, J.Z. Zhou,

More information

WYSE Academic Challenge Sectional Mathematics 2006 Solution Set

WYSE Academic Challenge Sectional Mathematics 2006 Solution Set WYSE Academic Challenge Sectinal 006 Slutin Set. Cect answe: e. mph is 76 feet pe minute, and 4 mph is 35 feet pe minute. The tip up the hill takes 600/76, 3.4 minutes, and the tip dwn takes 600/35,.70

More information

Analytical Solution to Diffusion-Advection Equation in Spherical Coordinate Based on the Fundamental Bloch NMR Flow Equations

Analytical Solution to Diffusion-Advection Equation in Spherical Coordinate Based on the Fundamental Bloch NMR Flow Equations Intenatinal Junal f heetical and athematical Phsics 5, 5(5: 4-44 OI:.593/j.ijtmp.555.7 Analtical Slutin t iffusin-advectin Equatin in Spheical Cdinate Based n the Fundamental Blch N Flw Equatins anladi

More information

Proceedings of the 11th WSEAS International Conference on Automatic Control, Modelling and Simulation

Proceedings of the 11th WSEAS International Conference on Automatic Control, Modelling and Simulation Tempeatue measuement in contact pantogaph - AC contact line Constantin-Floin OCOLEANU *, Ioan POPA *, Gheoghe MANOLEA **, Alin-Iulian DOLAN * Electical Appaatus and Technologies *, Electomechanical **

More information

5.1 Moment of a Force Scalar Formation

5.1 Moment of a Force Scalar Formation Outline ment f a Cuple Equivalent System Resultants f a Fce and Cuple System ment f a fce abut a pint axis a measue f the tendency f the fce t cause a bdy t tate abut the pint axis Case 1 Cnside hizntal

More information

On the Micropolar Fluid Flow through Porous Media

On the Micropolar Fluid Flow through Porous Media Pceedings f the th WEA Int. Cnf. n MATHEMATICAL METHOD, COMPUTATIONAL TECHNIQUE AND INTELLIGENT YTEM On the Micpla Fluid Flw thugh Pus Media M.T. KAMEL 3, D. ROACH, M.H. HAMDAN,3 Depatment f Mathematical

More information

Experimental and theoretical characterization of Li 2 TiO 3 and Li 4 SiO 4 pebbles

Experimental and theoretical characterization of Li 2 TiO 3 and Li 4 SiO 4 pebbles Experimental and theoretical characterization of Li 2 TiO 3 and Li 4 SiO 4 s D. Aquaro 1 N. Zaccari ABSTRACT Dipartimento di Ingegneria Meccanica Nucleare e della Produzione University of Pisa (Italy)

More information

Experimentally Derived Resistivity for Dielectric Samples from the CRRES Internal Discharge Monitor

Experimentally Derived Resistivity for Dielectric Samples from the CRRES Internal Discharge Monitor Utah State Univesity DigitalCmmns@USU All Physics Faculty Publicatins Physics 10-2006 Expeimentally Deived Resistivity f Dielectic Samples fm the CRRES Intenal Dischage Mnit Nelsn W. Geen A. Rbb Fedeicksn

More information

2 E. on each of these two surfaces. r r r r. Q E E ε. 2 2 Qencl encl right left 0

2 E. on each of these two surfaces. r r r r. Q E E ε. 2 2 Qencl encl right left 0 Ch : 4, 9,, 9,,, 4, 9,, 4, 8 4 (a) Fom the diagam in the textbook, we see that the flux outwad though the hemispheical suface is the same as the flux inwad though the cicula suface base of the hemisphee

More information

DYNAMIC MODELLING OF N-CARDAN TRANSMISSIONS WITH SHAFTS IN SPATIAL CONFIGURATION. Part II. THE ALGORITHM OF DYNAMIC MODELLING

DYNAMIC MODELLING OF N-CARDAN TRANSMISSIONS WITH SHAFTS IN SPATIAL CONFIGURATION. Part II. THE ALGORITHM OF DYNAMIC MODELLING Fascicle f Management and Technlgical Engineering, Vlume VI (XVI), 7 DYNAMIC MODELLING OF N-CARDAN TRANSMISSIONS WITH SHAFTS IN SPATIAL CONFIGURATION. Part II. THE ALGORITHM OF DYNAMIC MODELLING Cdrua

More information

Research Article EXPERIMENTAL STUDY OF HEAT TRANSFER CHARACTERISTICS OF STAINLESS STEEL FIBROUS FLOW INSULATOR

Research Article EXPERIMENTAL STUDY OF HEAT TRANSFER CHARACTERISTICS OF STAINLESS STEEL FIBROUS FLOW INSULATOR Tansactions of the TSME (16) Vol. 4, No. 2, 148 155 Jounal of seach and Applications in Mechanical Engineeing Copyight 16 by TSME ISSN 2229-2152 pint DOI: 1.14456/jame.16.15 seach Aticle EXPERIMENTAL STUDY

More information

Phy 213: General Physics III

Phy 213: General Physics III Phy 1: Geneal Physics III Chapte : Gauss Law Lectue Ntes E Electic Flux 1. Cnside a electic field passing thugh a flat egin in space w/ aea=a. The aea vect ( A ) with a magnitude f A and is diected nmal

More information

Water flows through the voids in a soil which are interconnected. This flow may be called seepage, since the velocities are very small.

Water flows through the voids in a soil which are interconnected. This flow may be called seepage, since the velocities are very small. Wate movement Wate flows though the voids in a soil which ae inteconnected. This flow may be called seepage, since the velocities ae vey small. Wate flows fom a highe enegy to a lowe enegy and behaves

More information

Materials selection The materials index

Materials selection The materials index MME445: Lectue 20 Mateials selection The mateials index A. K. M. B. Rashid Pofesso, Depatment of MME BUET, Dhaka Leaning Objectives Knowledge & Undestanding Elementay knowledge of how to expess design

More information

Analysis of thermal stratified storage tank

Analysis of thermal stratified storage tank ARCHIVES OF ELECRICAL ENGINEERING VOL. 66(3), pp. 63-64 (07) DOI 0.55/aee-07-0048 Analysis of themal statified stoage tank ROBER SMUSZ, PAWEŁ KIELAN, DAMIAN MAZUR 3 Depatment of hemodynamics and Fluid

More information

Consider the simple circuit of Figure 1 in which a load impedance of r is connected to a voltage source. The no load voltage of r

Consider the simple circuit of Figure 1 in which a load impedance of r is connected to a voltage source. The no load voltage of r 1 Intductin t Pe Unit Calculatins Cnside the simple cicuit f Figue 1 in which a lad impedance f L 60 + j70 Ω 9. 49 Ω is cnnected t a vltage suce. The n lad vltage f the suce is E 1000 0. The intenal esistance

More information

Summary chapter 4. Electric field s can distort charge distributions in atoms and molecules by stretching and rotating:

Summary chapter 4. Electric field s can distort charge distributions in atoms and molecules by stretching and rotating: Summa chapte 4. In chapte 4 dielectics ae discussed. In thse mateials the electns ae nded t the atms mlecules and cannt am fee thugh the mateial: the electns in insulats ae n a tight leash and all the

More information

Section 4.2 Radians, Arc Length, and Area of a Sector

Section 4.2 Radians, Arc Length, and Area of a Sector Sectin 4.2 Radian, Ac Length, and Aea f a Sect An angle i fmed by tw ay that have a cmmn endpint (vetex). One ay i the initial ide and the the i the teminal ide. We typically will daw angle in the cdinate

More information

transformation Earth V-curve (meridian) λ Conical projection. u,v curves on the datum surface projected as U,V curves on the projection surface

transformation Earth V-curve (meridian) λ Conical projection. u,v curves on the datum surface projected as U,V curves on the projection surface . CONICAL PROJECTIONS In elementay texts on map pojections, the pojection sufaces ae often descibed as developable sufaces, such as the cylinde (cylindical pojections) and the cone (conical pojections),

More information

THERMAL PROPERTIES OF FRACTAL STRUCTURE MATERIALS

THERMAL PROPERTIES OF FRACTAL STRUCTURE MATERIALS HERMAL PROPERIES OF FRACAL SRUCURE MAERIALS Oldřich Zmeškal, Mioslav Buchníček, Matin Nežádal Pavla Štefková, Radek Capoušek Institute of Physical and Applied Chemisty, Faculty of Chemisty, Bno Univesity

More information

Experience from PV system performence including comparison of on-roof and façade systems. (Case study on BIPV systems.)

Experience from PV system performence including comparison of on-roof and façade systems. (Case study on BIPV systems.) Expeience fom PV system pefomence including compaison of on-oof and façade systems. (Case study on BIPV systems.) Vitezslav Benda CTU Pague, Faculty of Electical Engineeing Intelligent enegy management

More information

Velocimetry Techniques and Instrumentation

Velocimetry Techniques and Instrumentation AeE 344 Lectue Notes Lectue # 05: elocimety Techniques and Instumentation D. Hui Hu Depatment of Aeospace Engineeing Iowa State Univesity Ames, Iowa 500, U.S.A Methods to Measue Local Flow elocity - Mechanical

More information

LINEAR PLATE BENDING

LINEAR PLATE BENDING LINEAR PLATE BENDING 1 Linea plate bending A plate is a body of which the mateial is located in a small egion aound a suface in the thee-dimensional space. A special suface is the mid-plane. Measued fom

More information

AIR FORCE RESEARCH LABORATORY

AIR FORCE RESEARCH LABORATORY AIR FORC RSARCH LABORATORY The xtinctin Theem as an xample f Reseach Vistas in Mathematical Optics Mach Richad A. Albanese Infmatin Opeatins and Applied Mathematics Human ffectiveness Diectate Bks City-Base

More information

Chapter Introduction to Finite Element Methods

Chapter Introduction to Finite Element Methods Chapte 1.4 Intoduction to Finite Element Methods Afte eading this chapte, you should e ale to: 1. Undestand the asics of finite element methods using a one-dimensional polem. In the last fifty yeas, the

More information

ELECTRIC & MAGNETIC FIELDS I (STATIC FIELDS) ELC 205A

ELECTRIC & MAGNETIC FIELDS I (STATIC FIELDS) ELC 205A LCTRIC & MAGNTIC FILDS I (STATIC FILDS) LC 05A D. Hanna A. Kils Assciate Pfess lectnics & Cmmnicatins ngineeing Depatment Faclty f ngineeing Cai Univesity Fall 0 f Static lecticity lectic & Magnetic Fields

More information

See the solution to Prob Ans. Since. (2E t + 2E c )ch - a. (s max ) t. (s max ) c = 2E c. 2E c. (s max ) c = 3M bh 2E t + 2E c. 2E t. h c.

See the solution to Prob Ans. Since. (2E t + 2E c )ch - a. (s max ) t. (s max ) c = 2E c. 2E c. (s max ) c = 3M bh 2E t + 2E c. 2E t. h c. *6 108. The beam has a ectangula coss section and is subjected to a bending moment. f the mateial fom which it is made has a diffeent modulus of elasticity fo tension and compession as shown, detemine

More information

which represents a straight line whose slope is C 1.

which represents a straight line whose slope is C 1. hapte, Slutin 5. Ye, thi claim i eanable ince in the abence any heat eatin the ate heat tane thugh a plain wall in teady peatin mut be cntant. But the value thi cntant mut be ze ince ne ide the wall i

More information

Chapter 2 ONE DIMENSIONAL STEADY STATE CONDUCTION. Chapter 2 Chee 318 1

Chapter 2 ONE DIMENSIONAL STEADY STATE CONDUCTION. Chapter 2 Chee 318 1 hapte ONE DIMENSIONAL SEADY SAE ONDUION hapte hee 38 HEA ONDUION HOUGH OMPOSIE EANGULA WALLS empeatue pofile A B X X 3 X 3 4 X 4 Χ A Χ B Χ hapte hee 38 hemal conductivity Fouie s law ( is constant) A A

More information

Lecture 7 Further Development of Theory and Applications

Lecture 7 Further Development of Theory and Applications P4 Stress and Strain Dr. A.B. Zavatsk HT08 Lecture 7 Further Develpment f Ther and Applicatins Hke s law fr plane stress. Relatinship between the elastic cnstants. lume change and bulk mdulus. Spherical

More information

CS579 - Homework 2. Tu Phan. March 10, 2004

CS579 - Homework 2. Tu Phan. March 10, 2004 I! CS579 - Hmewk 2 Tu Phan Mach 10, 2004 1 Review 11 Planning Pblem and Plans The planning pblem we ae cnsideing is a 3-tuple descibed in the language whse syntax is given in the bk, whee is the initial

More information

Combustion Chamber. (0.1 MPa)

Combustion Chamber. (0.1 MPa) ME 354 Tutial #10 Winte 001 Reacting Mixtues Pblem 1: Detemine the mle actins the pducts cmbustin when ctane, C 8 18, is buned with 00% theetical ai. Als, detemine the dew-pint tempeatue the pducts i the

More information

From Gravitational Collapse to Black Holes

From Gravitational Collapse to Black Holes Fom Gavitational Collapse to Black Holes T. Nguyen PHY 391 Independent Study Tem Pape Pof. S.G. Rajeev Univesity of Rocheste Decembe 0, 018 1 Intoduction The pupose of this independent study is to familiaize

More information

Higher Mathematics Booklet CONTENTS

Higher Mathematics Booklet CONTENTS Higher Mathematics Bklet CONTENTS Frmula List Item Pages The Straight Line Hmewrk The Straight Line Hmewrk Functins Hmewrk 3 Functins Hmewrk 4 Recurrence Relatins Hmewrk 5 Differentiatin Hmewrk 6 Differentiatin

More information

REPORT ITU-R SA Protection of the space VLBI telemetry link

REPORT ITU-R SA Protection of the space VLBI telemetry link Rep. ITU-R SA.65 REPORT ITU-R SA.65 Ptectin f the space VLBI telemety link CONTENTS Page Intductin... Space VLBI system.... Space VLBI telemety signal, nise and intefeence..... Signal... 3.. Nise and intefeence...

More information

OPERATIONAL AMPLIFIERS

OPERATIONAL AMPLIFIERS PEATINAL AMPLIFIES Why do we study them at ths pont???. pamps are ery useful electronc components. We hae already the tools to analyze practcal crcuts usng pamps 3. The lnear models for pamps nclude dependent

More information

Spatial Development of Viscous Flow Induced by Wave Propagation over Vortex Ripples

Spatial Development of Viscous Flow Induced by Wave Propagation over Vortex Ripples Intenational Congess on Envionmental Modelling and Softwae Bigham Young Univesity BYU ScholasAchive 4th Intenational Congess on Envionmental Modelling and Softwae - Bacelona, Catalonia, Spain - July 8

More information

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS The 8 th Intenational Confeence of the Slovenian Society fo Non-Destuctive Testing»pplication of Contempoay Non-Destuctive Testing in Engineeing«Septembe 1-3, 5, Potoož, Slovenia, pp. 17-1 MGNETIC FIELD

More information

Long-range stress re-distribution resulting from damage in heterogeneous media

Long-range stress re-distribution resulting from damage in heterogeneous media Long-ange stess e-distibution esulting fom damage in heteogeneous media Y.L.Bai (1), F.J.Ke (1,2), M.F.Xia (1,3) X.H.Zhang (1) and Z.K. Jia (1) (1) State Key Laboatoy fo Non-linea Mechanics (LNM), Institute

More information