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

Size: px
Start display at page:

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

Transcription

1 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 Ci + i t Upn epesenting instantaneus cncentatin by the su f the tie aveaged and fluctuatin pat Ci = C% i + Ci, we get the fllwing equatin f the tie aveaged cncentatin C % i. C ~ i ~ + vci = ( Di Ci < v Ci > ) + ~ i τ In the abve bth ~ and < > epesent enseble ( tie) aveaged values. This equies a del f the velcity cncentatin css celatin and f the ate. < vci >= Dt C % i % = k < CC >= k < ( C + C)( C + C) > ~ ~ k C C + < C C > + < C C > + < C y definitin = [ C > ] < C >= < C >= 0 a% % = k CC % % + < CC > = b hgeneus ate at lcal css celatin f ean ate = + tie aveaged cncentatin cncentatin fluctuatin ean ate < hgeneus ean ate s k < C C > C % C % t keep ate finite. Epeiental veificatin sught n tubulence effects f: - instantaneus - apid - slw eactins Cnside that in a given syste the iing ate can be established by unning instantaneus eactins at β =. Then = ()

2 CHE 52 - CHPTE Sping 2005 If tubulence paaetes wee nt easued, ne can deteine vs z i.e ( z/ u ). Nw the ate is due entiely t iing and ne can wite d Cu k CC dz = = (2) & ( ) C = C = C (3) whee C is the css-sectinal aveage. Thus k f the syste can be deteined ve a ange f eynlds nubes. Nw the chaacteistic eactin nube is k NM = (4) k N M >> N M > N M << instantaneus eactin apid eactin slw eactin The fllwing eactins wee cnsideed: k (L/l s) at 30 C. HCl + NaOH instantaneus 2. HCl + LiOH instantaneus 3. (COOH) 2 + 2LiOH 0 alic acid 4. HCOOH + LiOH fic acid 5. CO 2 + 2NaOH CO 2 + n NH 3 (n=-2) HCOOCH 3 + NaOH ethylfate t stichietic feed f eactants, β =, and f an instantaneus eactin (such as the fist tw listed abve) f eq (2) it fllws that d ( ) 2 dz = (5) u kc z = z = 0 Integatin f (5) & (5a) yields kc = + u ( z z ) Epeiental eact with 00 tubes, ID = inches (0.3 c) 5 in lng was used. Tubes wee pessed int hles f a /4" diaete disk that clsed the uppe end f the /4" (3.75 c) diaete (5a) (6) 2

3 CHE 52 - CHPTE Sping 2005 lucite tubula eact. eactants ae fed t altenate tubes with e = 3,700 in tubes and 5,000 in the eact. Jet velcity = 6 ean eact velcity. u 5.85 in/ s = c/ s. eactant cncentatin had t be nited. Deinized wate was used. eactant caying steas ae thestated at 29.9 C in a theal bath. eactin pgess is nited by adiabatic tepeatue ise. C ρc p = H ρc p = H T T (7) (8) T T is easued by a cppe cnstant in glass shielded thecuple (30 gauge) whse efeence junctin is in ne f the feed steas just befe iing. Effective tip diaete was in (0.5 c). Measueents wee veified with fine pbes. lind uns with pue wate wee als dne and the signal was subtacted (heat f fictin, heat lsses, etc.). Measued adial T pfiles wee flat s T can be easued as equal t the cente line tepeatue. ll fu vey apid eactins behaved as instantaneus and pduced at fied β = the sae cnvesin vs distance cuve. FIGUE : eactant cnvesin f vey apid eactins as a functin f distance f stichietic feeds (β = ) [F Vassilats and Tu, IChE J., 666 (965)] FCTIONL CONVESION, 3

4 CHE 52 - CHPTE Sping 2005 Least squaes fit f eq (6) at β = t the data gives 9.24( z 0.44) ) ; z 0.44 in = + > (9) Ecellent staight line is btained when vs z is pltted ecept at vey fist few data pints z < F eq (9), based n they, we cnclude that the degee f unaccplished iing is given by a hypeblic decay law. = ; z > ( z ) (0) Cpaisn f fula (6) and (9) yields k 305a L = bc ls () Nw f nn-stichietic feeds the they pedicts [eq (24) and (22) f pevius pat] = + ( β ) + g γ t (2) whee γ t is given by the slutin f β g β = ( γ ) t (3) whee g( ) = iefc (4) 2 2 ac β = (5) bc Nw we knw f eq (0). Cpaisn f data and theetical pedictins was ecellent f β in the inteval (,0). 4

5 CHE 52 - CHPTE Sping 2005 FIGUE 2: Factinal cnvesin vs. accplished iing, vey apid eactins. Nw ne tested the assuptin f 2nd de iing law at β F β eq (5) beces d dz b a ( )( β ) u = k C Upn integatin this yields: ( / ) k b a C ln = l nβ ( β ) ( z z) (7) u Plts f l n vs z did yield staight lines f all instantaneus eactins. The slpes f the lines evealed 305 k = ψ ( β ) (8) b C a 5

6 CHE 52 - CHPTE Sping 2005 whee f β =, ψ = ; and f β = 0, ψ = 0.3. ased n these findings we see that N M N M b C k = a k 305ψ β = (9) ( ) k Since k 0,000 t 20,000 L/l s, indeed all f the fist 4 eactins ae instantaneus. One shuld ecall that the 2nd de decay law f geneal law. is the peculiaity f the iing device, nt a NOTE: ial dispesin effects ae negligible and PF fulas (eq 6) pduce the desied esult. F the CO 2 + 2NaOH eactin N M = 0.5 t 0 If we assue = KC C (20) Plt f l n b K( β ) C ln n a = l β ( z z ) (2) u yields staight lines but K = K( β ). F this paticula eactin k = 2,400 (L/l s). L efe we fund f instantaneus eactins that at β = 3.88 we have k = 9, 400. l s Then, L N M =.30 f the cabn diide eactin with sdiu hydide and we get K = 2770 l s. Siilaly, at L β =.26, k = 9,700( L / l s), N M = 0.63 and we find K = 3420 l s Thus, K < k, k k 6

7 CHE 52 - CHPTE Sping 2005 F CO 2 + NH 3 - the sae phenenn is bseved k = 585 (L/l s) k( L/ l s) N K( L/ l s) β = 2. 24, β = , = and the hgeneus ate law hlds with K= k = 47. (L/l s) and z 0 = 0. Hgeneus ate eactin is bseved as 0. 3 F the Methyl fate - sdiu hydide eactin ( N M 0 ) Thughut this eact the ean ate is a fied factin, K/k, f the hgeneus ean ate even thugh the fluid is becing e hgeneus as z inceases. If PF assuptins ae O.K. then these values CC K CC = k vay f 0.72 at β =.26 t 0.78 at β = 3.88 f CO2 + 2 NaOH., and ae lwe f CO 2 + nnh 3 i.e. 0 f β = 2.t 0.43 at β = 0. F inteediate eactins thee is n clea patten egading the value f the appaent ate cnstant K t be used. The appiate epessin + is valid nly in the tw liits as K k k NM N M N 0 M The actual K, K act is less than K - estiated by abve fula f apid eactins. Thus k = + = + M K k k k k K = act + N > K M ( N ) 7

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

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

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

School of Chemical & Biological Engineering, Konkuk University

School of Chemical & Biological Engineering, Konkuk University Schl f Cheical & Bilgical Engineeing, Knkuk Univesity Lectue 7 Ch. 2 The Fist Law Thecheisty Pf. Y-Sep Min Physical Cheisty I, Sping 2008 Ch. 2-2 The study f the enegy tansfeed as heat duing the cuse f

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

ME 236 Engineering Mechanics I Test #4 Solution

ME 236 Engineering Mechanics I Test #4 Solution ME 36 Enineein Mechnics I est #4 Slutin Dte: id, M 14, 4 ie: 8:-1: inutes Instuctins: vein hptes 1-13 f the tetbk, clsed-bk test, clcults llwed. 1 (4% blck ves utwd ln the slt in the pltf with speed f

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

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

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

ATMO 551a Fall 08. Diffusion

ATMO 551a Fall 08. Diffusion Diffusion Diffusion is a net tanspot of olecules o enegy o oentu o fo a egion of highe concentation to one of lowe concentation by ando olecula) otion. We will look at diffusion in gases. Mean fee path

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

Hotelling s Rule. Therefore arbitrage forces P(t) = P o e rt.

Hotelling s Rule. Therefore arbitrage forces P(t) = P o e rt. Htelling s Rule In what fllws I will use the tem pice t dente unit pfit. hat is, the nminal mney pice minus the aveage cst f pductin. We begin with cmpetitin. Suppse that a fim wns a small pa, a, f the

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

Physics 321 Solutions for Final Exam

Physics 321 Solutions for Final Exam Page f 8 Physics 3 Slutins fr inal Exa ) A sall blb f clay with ass is drpped fr a height h abve a thin rd f length L and ass M which can pivt frictinlessly abut its center. The initial situatin is shwn

More information

torr ~tirru 'V Q Hz N/m 2 EQUIPMENT z a r 1 INTRODUCTION

torr ~tirru 'V Q Hz N/m 2 EQUIPMENT z a r 1 INTRODUCTION l @1~ 8 ~tiu ilf'@m W@~(Q) H~W t N-J ERMEER Delft Univesity f Technlgy, The Nethelands a~ SYNOPSS As a cntinuatin f ealie wk, velcities have been easued in the nea wake f a del t in the wind tunnel By

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

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

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

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

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

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

1. Show that if the angular momentum of a boby is determined with respect to an arbitrary point A, then. r r r. H r A can be expressed by H r r r r

1. Show that if the angular momentum of a boby is determined with respect to an arbitrary point A, then. r r r. H r A can be expressed by H r r r r 1. Shw that if the angula entu f a bb is deteined with espect t an abita pint, then H can be epessed b H = ρ / v + H. This equies substituting ρ = ρ + ρ / int H = ρ d v + ρ ( ω ρ ) d and epanding, nte

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

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

March 15. Induction and Inductance Chapter 31

March 15. Induction and Inductance Chapter 31 Mach 15 Inductin and Inductance Chapte 31 > Fces due t B fields Lentz fce τ On a mving chage F B On a cuent F il B Cuent caying cil feels a tque = µ B Review > Cuents geneate B field Bit-Savat law = qv

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

Lecture 2: Single-particle Motion

Lecture 2: Single-particle Motion Lecture : Single-particle Mtin Befre we start, let s l at Newtn s 3 rd Law Iagine a situatin where frces are nt transitted instantly between tw bdies, but rather prpagate at se velcity c This is true fr

More information

Physics 2A Chapter 10 - Moment of Inertia Fall 2018

Physics 2A Chapter 10 - Moment of Inertia Fall 2018 Physics Chapte 0 - oment of netia Fall 08 The moment of inetia of a otating object is a measue of its otational inetia in the same way that the mass of an object is a measue of its inetia fo linea motion.

More information

Chapter 2: Estuarine Salinity Structure and Circulation

Chapter 2: Estuarine Salinity Structure and Circulation Chapte : Estuaine Salinity Stuctue and Ciculatin W.R. Geye, Wds Hle Oceangaphic Institutin.. The Hizntal Salinity Gadient Estuaies shw a geat divesity f size, shape, depth, and fcing chaacteistics, but

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

AN UPPER BOUND SOLUTION OF BACKWARD TUBE EXTRUSION PROCESS THROUGH CURVED PUNCHES

AN UPPER BOUND SOLUTION OF BACKWARD TUBE EXTRUSION PROCESS THROUGH CURVED PUNCHES Acta Metallugica Slvaca, l., 4, N., p. 5-49 5 AN UPPER BOUND SOLUTION OF BACKWARD TUBE EXTRUSION PROCESS THROUGH CURED PUNCHES Heshatllah Haghighat *, Ghla Reza Asgai Mechanical Engineeing Depatent, Razi

More information

PDF Created with deskpdf PDF Writer - Trial ::

PDF Created with deskpdf PDF Writer - Trial :: A APPENDIX D TRIGONOMETRY Licensed to: jsamuels@bmcc.cun.edu PDF Ceated with deskpdf PDF Wite - Tial :: http://www.docudesk.com D T i g o n o m e t FIGURE a A n g l e s Angles can be measued in degees

More information

EPr over F(X} AA+ A+A. For AeF, a generalized inverse. ON POLYNOMIAL EPr MATRICES

EPr over F(X} AA+ A+A. For AeF, a generalized inverse. ON POLYNOMIAL EPr MATRICES Intenat. J. Hath. & Math. S. VOL. 15 NO. 2 (1992) 261-266 ON POLYNOMIAL EP MATRICES 261 AR. MEENAKSHI and N. ANANOAM Depatment f Mathematics, Annamalai Univeslty, Annamalainaga- 68 2, Tamll Nadu, INDIA.

More information

EN40: Dynamics and Vibrations. Midterm Examination Tuesday March

EN40: Dynamics and Vibrations. Midterm Examination Tuesday March EN4: Dynaics and Vibations Midte Exaination Tuesday Mach 8 16 School of Engineeing Bown Univesity NME: Geneal Instuctions No collaboation of any kind is peitted on this exaination. You ay bing double sided

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

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

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

ME 3600 Control Systems Frequency Domain Analysis

ME 3600 Control Systems Frequency Domain Analysis ME 3600 Contol Systems Fequency Domain Analysis The fequency esponse of a system is defined as the steady-state esponse of the system to a sinusoidal (hamonic) input. Fo linea systems, the esulting steady-state

More information

CHAPTER 17. Solutions for Exercises. Using the expressions given in the Exercise statement for the currents, we have

CHAPTER 17. Solutions for Exercises. Using the expressions given in the Exercise statement for the currents, we have CHATER 7 Slutin f Execie E7. F Equatin 7.5, we have B gap Ki ( t ) c( θ) + Ki ( t ) c( θ 0 ) + Ki ( t ) c( θ 40 a b c ) Uing the expein given in the Execie tateent f the cuent, we have B gap K c( ωt )c(

More information

3.1 Random variables

3.1 Random variables 3 Chapte III Random Vaiables 3 Random vaiables A sample space S may be difficult to descibe if the elements of S ae not numbes discuss how we can use a ule by which an element s of S may be associated

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

Examiner: Dr. Mohamed Elsharnoby Time: 180 min. Attempt all the following questions Solve the following five questions, and assume any missing data

Examiner: Dr. Mohamed Elsharnoby Time: 180 min. Attempt all the following questions Solve the following five questions, and assume any missing data Benha University Cllege f Engineering at Banha Department f Mechanical Eng. First Year Mechanical Subject : Fluid Mechanics M111 Date:4/5/016 Questins Fr Final Crrective Examinatin Examiner: Dr. Mhamed

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

9.2 Reaction rate and rate equation

9.2 Reaction rate and rate equation 9.2.1 Expession of eaction ate The ate () of a chemical eaction is defined as the concentation change of a eactant o a poduct pe unit time. mean ate [A] c c = t t t 2 1 2 1 c c 1 instantaneous ate: Physical

More information

Tidal forces. m r. m 1 m 2. x r 2. r 1

Tidal forces. m r. m 1 m 2. x r 2. r 1 Tidal foces Befoe we look at fee waves on the eath, let s fist exaine one class of otion that is diectly foced: astonoic tides. Hee we will biefly conside soe of the tidal geneating foces fo -body systes.

More information

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

University of Pisa. N. Zaccari, D. Aquaro. Pebble Beds. - ITALY - Department of Mechanical, Nuclear and Production Engineering 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 Cntents f Pesentatin This pesentatin descibes the them-mechanical

More information

1121 T Question 1

1121 T Question 1 1121 T1 2008 Question 1 ( aks) You ae cycling, on a long staight path, at a constant speed of 6.0.s 1. Anothe cyclist passes you, tavelling on the sae path in the sae diection as you, at a constant speed

More information

Solution: (a) C 4 1 AI IC 4. (b) IBC 4

Solution: (a) C 4 1 AI IC 4. (b) IBC 4 C A C C R A C R C R C sin 9 sin. A cuent f is maintaine in a single cicula lp f cicumfeence C. A magnetic fiel f is iecte paallel t the plane f the lp. (a) Calculate the magnetic mment f the lp. (b) What

More information

1 Similarity Analysis

1 Similarity Analysis ME43A/538A/538B Axisymmetic Tubulent Jet 9 Novembe 28 Similaity Analysis. Intoduction Conside the sketch of an axisymmetic, tubulent jet in Figue. Assume that measuements of the downsteam aveage axial

More information

Compressibility Effects

Compressibility Effects Definitin f Cmpressibility All real substances are cmpressible t sme greater r lesser extent; that is, when yu squeeze r press n them, their density will change The amunt by which a substance can be cmpressed

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

Radiation Resistance of System G( Iron Torus is not used as we can see ) ( ) 2

Radiation Resistance of System G( Iron Torus is not used as we can see ) ( ) 2 THE FNAL NVESTGATON ON TORS EXPERMENT N AQNO S SET P n the llwing invetigatin, we ae ging t exaine the equatin Syte G, accding t Pe Aquin clai. THE EQATONS FOR THE TORS EXPERMENT ARE THE FOLLOW: Velcity

More information

Lim f (x) e. Find the largest possible domain and its discontinuity points. Why is it discontinuous at those points (if any)?

Lim f (x) e. Find the largest possible domain and its discontinuity points. Why is it discontinuous at those points (if any)? THESE ARE SAMPLE QUESTIONS FOR EACH OF THE STUDENT LEARNING OUTCOMES (SLO) SET FOR THIS COURSE. SLO 1: Understand and use the cncept f the limit f a functin i. Use prperties f limits and ther techniques,

More information

Centripetal Force OBJECTIVE INTRODUCTION APPARATUS THEORY

Centripetal Force OBJECTIVE INTRODUCTION APPARATUS THEORY Centipetal Foce OBJECTIVE To veify that a mass moving in cicula motion expeiences a foce diected towad the cente of its cicula path. To detemine how the mass, velocity, and adius affect a paticle's centipetal

More information

Inverse Square Law and Polarization

Inverse Square Law and Polarization Invese Squae Law and Polaization Objectives: To show that light intensity is invesely popotional to the squae of the distance fom a point light souce and to show that the intensity of the light tansmitted

More information

A perturbation density functional theory for the competition between inter and intramolecular association

A perturbation density functional theory for the competition between inter and intramolecular association petubatin density functinal they f the cpetitin between inte and intalecula assciatin Bennett D. Chapan a leand J. Gacía-Cuélla b and Walte G. Chapan a a Depatent f Cheical and Bilecula Engineeing Rice

More information

Lecture 23: Central Force Motion

Lecture 23: Central Force Motion Lectue 3: Cental Foce Motion Many of the foces we encounte in natue act between two paticles along the line connecting the Gavity, electicity, and the stong nuclea foce ae exaples These types of foces

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

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

Measurement of Residual Stress/Strain (Using Strain Gages and the Hole Drilling Method) Summary of Discussion in Section 8.9

Measurement of Residual Stress/Strain (Using Strain Gages and the Hole Drilling Method) Summary of Discussion in Section 8.9 Mesuement f Residul Stess/Stin (Using Stin Gges nd the Hle Dilling Methd) Summy f Discussin in Sectin 8.9 The Hle Dilling Methd Is Bsed On: () Stess tnsfmtin equtins τ x' x' y' y' x' y' xx xx cs sin sin

More information

CHAPTER 5: Circular Motion; Gravitation

CHAPTER 5: Circular Motion; Gravitation CHAPER 5: Cicula Motion; Gavitation Solution Guide to WebAssign Pobles 5.1 [1] (a) Find the centipetal acceleation fo Eq. 5-1.. a R v ( 1.5 s) 1.10 1.4 s (b) he net hoizontal foce is causing the centipetal

More information

Theory and Calibration Procedures for the Use of a Rotameter

Theory and Calibration Procedures for the Use of a Rotameter T I 4 3 5 : T O S H E R I S L I N G O U R S E ppendix F Theoy and alibation ocedues o the Use o a Rotaete F. Noenclatue = coss-sectional aea o the loat = annula aea between the cicueence o the loat and

More information

Phys 201A. Homework 5 Solutions

Phys 201A. Homework 5 Solutions Phys 201A Homewok 5 Solutions 3. In each of the thee cases, you can find the changes in the velocity vectos by adding the second vecto to the additive invese of the fist and dawing the esultant, and by

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

Equations to Calculate Characteristic Frequencies of Multiple Chamber Aligned in Parallel Cavity Resonator (MCAP-CR)

Equations to Calculate Characteristic Frequencies of Multiple Chamber Aligned in Parallel Cavity Resonator (MCAP-CR) MCAPE Equations to Calculate Chaacteistic Fequencies of Multiple Chabe Aligne in Paallel Cavity Resonato (MCAP-CR) Shigeu Suzui Mach, (Revise in ovebe, ). Peface It is necessay to solve the equations of

More information

ACE Engineering Academy

ACE Engineering Academy TEST ID: 0 ACE Engineeing Acadey Hydeabad Deli Bpal une Bubaneswa Bengaluu Lucknw atna Cennai ijayawada isakapatna Tiupati Kukatpally Klkata H.O: 0, II Fl, Raan laza, Opp. Metdist Scl, Abids, Hydeabad

More information

6 PROBABILITY GENERATING FUNCTIONS

6 PROBABILITY GENERATING FUNCTIONS 6 PROBABILITY GENERATING FUNCTIONS Cetain deivations pesented in this couse have been somewhat heavy on algeba. Fo example, detemining the expectation of the Binomial distibution (page 5.1 tuned out to

More information

UIUC Physics 435 EM Fields & Sources I Fall Semester, 2007 Lecture Notes 14 Prof. Steven Errede LECTURE NOTES 14

UIUC Physics 435 EM Fields & Sources I Fall Semester, 2007 Lecture Notes 14 Prof. Steven Errede LECTURE NOTES 14 UIU Physics 45 EM Fields & Suces I Fall Seeste, 007 Lectue Ntes 4 Pf. Steven Eede LETURE NOTES 4 THE MAROSOPI MAGNETI FIELD ASSOIATED WITH THE RELATIVE MOTION OF AN ELETRIALLY-HARGED POINT-LIKE PARTILE

More information

From Maxwell s Eqs. and Newton s Laws to the Vlasov and Fokker-Planck Eqs.

From Maxwell s Eqs. and Newton s Laws to the Vlasov and Fokker-Planck Eqs. F Maxwell s Eqs. and Newtn s Laws t the Vlas and Fkke-Planck Eqs. Rbet A. Schill, J. Uniesity f Neada, Las Vegas Dept. f Electical and Cpute Engineeing 4505 Mayland Pakway; Bx 45406 Las Vegas, NV 89154-406

More information

DINGWALL ACADEMY NATIONAL QUALIFICATIONS. Mathematics Higher Prelim Examination 2009/2010 Paper 1 Assessing Units 1 & 2. Time allowed - 1 hour 30

DINGWALL ACADEMY NATIONAL QUALIFICATIONS. Mathematics Higher Prelim Examination 2009/2010 Paper 1 Assessing Units 1 & 2. Time allowed - 1 hour 30 INGWLL EMY Mathematics Higher Prelim Eaminatin 009/00 Paper ssessing Units & NTIONL QULIFITIONS Time allwed - hur 0 minutes Read carefull alculatrs ma NOT be used in this paper. Sectin - Questins - 0 (0

More information

Circular Orbits. and g =

Circular Orbits. and g = using analyse planetay and satellite motion modelled as unifom cicula motion in a univesal gavitation field, a = v = 4π and g = T GM1 GM and F = 1M SATELLITES IN OBIT A satellite is any object that is

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

CSTR - PFR - PBR

CSTR - PFR - PBR 1. Mole Balances o The Rate of Reaction, - o The Geneal Mole Balance Equation o Continuous low Reactos - CSTR (Continuous-Stied Tank Reacto) - PR (Tubula Reacto) - PBR (Packed-Bed Reacto) o Industial Reactos

More information

Unit 6 Practice Test. Which vector diagram correctly shows the change in velocity Δv of the mass during this time? (1) (1) A. Energy KE.

Unit 6 Practice Test. Which vector diagram correctly shows the change in velocity Δv of the mass during this time? (1) (1) A. Energy KE. Unit 6 actice Test 1. Which one of the following gaphs best epesents the aiation of the kinetic enegy, KE, and of the gaitational potential enegy, GE, of an obiting satellite with its distance fom the

More information

Chapter 13 Gravitation

Chapter 13 Gravitation Chapte 13 Gavitation In this chapte we will exploe the following topics: -Newton s law of gavitation, which descibes the attactive foce between two point masses and its application to extended objects

More information

FARADAY'S LAW. dates : No. of lectures allocated. Actual No. of lectures 3 9/5/09-14 /5/09

FARADAY'S LAW. dates : No. of lectures allocated. Actual No. of lectures 3 9/5/09-14 /5/09 FARADAY'S LAW No. of lectues allocated Actual No. of lectues dates : 3 9/5/09-14 /5/09 31.1 Faaday's Law of Induction In the pevious chapte we leaned that electic cuent poduces agnetic field. Afte this

More information

Study of C5/C6 isomerization on Pt/H-zeolite catalyst in industrial conditions

Study of C5/C6 isomerization on Pt/H-zeolite catalyst in industrial conditions Ovidius Univesity Annals of Chemisty Volume, Numbe, pp. -6, Study of / isomeization on Pt/H-zeolite catalyst in industial conditions Claudia Iina KONCSAG*, Ioan Alexandu TUTUN and Cistian SAFTA Ovidius

More information

Pre-Calculus Individual Test 2017 February Regional

Pre-Calculus Individual Test 2017 February Regional The abbreviatin NOTA means Nne f the Abve answers and shuld be chsen if chices A, B, C and D are nt crrect. N calculatr is allwed n this test. Arcfunctins (such as y = Arcsin( ) ) have traditinal restricted

More information

ENGI 4430 Parametric Vector Functions Page 2-01

ENGI 4430 Parametric Vector Functions Page 2-01 ENGI 4430 Parametric Vectr Functins Page -01. Parametric Vectr Functins (cntinued) Any nn-zer vectr r can be decmpsed int its magnitude r and its directin: r rrˆ, where r r 0 Tangent Vectr: dx dy dz dr

More information

Queuing Network Approximation Technique for Evaluating Performance of Computer Systems with Hybrid Input Source

Queuing Network Approximation Technique for Evaluating Performance of Computer Systems with Hybrid Input Source Int'l Conf. cientific Coputing CC'7 3 Queuing Netwok Appoxiation Technique fo Evaluating Pefoance of Copute ystes with Hybid Input ouce Nozoi iyaoto, Daisuke iyake, Kaoi Katsuata, ayuko Hiose, Itau Koike,

More information

Nuclear and Particle Physics - Lecture 20 The shell model

Nuclear and Particle Physics - Lecture 20 The shell model 1 Intoduction Nuclea and Paticle Physics - Lectue 0 The shell model It is appaent that the semi-empiical mass fomula does a good job of descibing tends but not the non-smooth behaviou of the binding enegy.

More information

Design of Analog Integrated Circuits

Design of Analog Integrated Circuits Design f Analg Integated Cicuits Opeatinal Aplifies Design f Analg Integated Cicuits Fall 01, D. Guxing Wang 1 Outline Mdel f Opeatinal Aplifies Tw Stage CMOS Op Ap Telescpic Op Ap Flded-Cascde Op Ap Refeence

More information

Chapter 5 Trigonometric Functions

Chapter 5 Trigonometric Functions Chapte 5 Tignmetic Functins Sectin 5.2 Tignmetic Functins 5-5. Angles Basic Teminlgy Degee Measue Standad Psitin Cteminal Angles Key Tems: vetex f an angle, initial side, teminal side, psitive angle, negative

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

Galactic Contraction and the Collinearity Principle

Galactic Contraction and the Collinearity Principle TECHNISCHE MECHANIK, Band 23, Heft 1, (2003), 21-28 Manuskipteingang: 12. August 2002 Galactic Contaction and the Collineaity Pinciple F.P.J. Rimott, FA. Salusti In a spial galaxy thee is not only a Keplefoce

More information

Introduction: A Generalized approach for computing the trajectories associated with the Newtonian N Body Problem

Introduction: A Generalized approach for computing the trajectories associated with the Newtonian N Body Problem A Generalized apprach fr cmputing the trajectries assciated with the Newtnian N Bdy Prblem AbuBar Mehmd, Syed Umer Abbas Shah and Ghulam Shabbir Faculty f Engineering Sciences, GIK Institute f Engineering

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

30 The Electric Field Due to a Continuous Distribution of Charge on a Line

30 The Electric Field Due to a Continuous Distribution of Charge on a Line hapte 0 The Electic Field Due to a ontinuous Distibution of hage on a Line 0 The Electic Field Due to a ontinuous Distibution of hage on a Line Evey integal ust include a diffeential (such as d, dt, dq,

More information

The Concept of the Effective Mass Tensor in GR. Clocks and Rods

The Concept of the Effective Mass Tensor in GR. Clocks and Rods The Concept of the Effective Mass Tenso in GR Clocks and Rods Miosław J. Kubiak Zespół Szkół Technicznych, Gudziądz, Poland Abstact: In the pape [] we pesented the concept of the effective ass tenso (EMT)

More information

1) p represents the number of holes present. We know that,

1) p represents the number of holes present. We know that, ECE650R : Reliability Physics f Nanelectrnic Devices Lecture 13 : Features f FieldDependent NBTI Degradatin Date : Oct. 11, 2006 Classnte : Saakshi Gangwal Review : Pradeep R. Nair 13.0 Review In the last

More information

KANTOROVICH TYPE INEQUALITIES FOR THE DIFFERENCE WITH TWO NEGATIVE PARAMETERS. Received April 13, 2010; revised August 18, 2010

KANTOROVICH TYPE INEQUALITIES FOR THE DIFFERENCE WITH TWO NEGATIVE PARAMETERS. Received April 13, 2010; revised August 18, 2010 Scientiae Matheaticae Japonicae Online, e-200, 427 439 427 KANTOROVICH TYPE INEQUALITIES FOR THE DIFFERENCE WITH TWO NEGATIVE PARAMETERS Young Ok Ki, Jun Ichi Fujii, Masatoshi Fujii + and Yuki Seo ++ Received

More information

CHAPTER 3. Section 1. Modeling Population Growth

CHAPTER 3. Section 1. Modeling Population Growth CHAPTER 3 Section 1. Modeling Population Gowth 1.1. The equation of the Malthusian model is Pt) = Ce t. Apply the initial condition P) = 1. Then 1 = Ce,oC = 1. Next apply the condition P1) = 3. Then 3

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

4F-5 : Performance of an Ideal Gas Cycle 10 pts

4F-5 : Performance of an Ideal Gas Cycle 10 pts 4F-5 : Perfrmance f an Cycle 0 pts An ideal gas, initially at 0 C and 00 kpa, underges an internally reversible, cyclic prcess in a clsed system. The gas is first cmpressed adiabatically t 500 kpa, then

More information

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations Phys-7 Lectue 17 Motional Electomotive Foce (emf) Induced Electic Fields Displacement Cuents Maxwell s Equations Fom Faaday's Law to Displacement Cuent AC geneato Magnetic Levitation Tain Review of Souces

More information

Markscheme May 2017 Calculus Higher level Paper 3

Markscheme May 2017 Calculus Higher level Paper 3 M7/5/MATHL/HP3/ENG/TZ0/SE/M Makscheme May 07 Calculus Highe level Pape 3 pages M7/5/MATHL/HP3/ENG/TZ0/SE/M This makscheme is the popety of the Intenational Baccalaueate and must not be epoduced o distibuted

More information

SPH4U Unit 6.3 Gravitational Potential Energy Page 1 of 9

SPH4U Unit 6.3 Gravitational Potential Energy Page 1 of 9 SPH4 nit 6.3 Gavitational Potential negy Page of Notes Physics ool box he gavitational potential enegy of a syste of two (spheical) asses is diectly popotional to the poduct of thei asses, and invesely

More information

Announcements 19 Nov 2009

Announcements 19 Nov 2009 Announceents 19 Nov 009 1. No class on Tuesday (Fiday instuction). Exa 4 stats today! a. Exa ends Tues Nov 4 (late fee afte 3 p) b. Coves Chaptes 9-1, HW 15-0 (but cuulative) c. Anticipated aveage tie:

More information

Electric Fields and Electric Forces

Electric Fields and Electric Forces Cpyight, iley 006 (Cutnell & Jhnsn 9. Ptential Enegy Chapte 9 mgh mgh GPE GPE Electic Fields and Electic Fces 9. Ptential Enegy 9. Ptential Enegy 9. The Electic Ptential Diffeence 9. The Electic Ptential

More information

ChE 471: LECTURE 4 Fall 2003

ChE 471: LECTURE 4 Fall 2003 ChE 47: LECTURE 4 Fall 003 IDEL RECTORS One f the key gals f chemical reactin engineering is t quantify the relatinship between prductin rate, reactr size, reactin kinetics and selected perating cnditins.

More information