SOLUTION. The reactor thermal output is related to the maximum heat flux in the hot channel by. Z( z ). The position of maximum heat flux ( z max
|
|
|
- Flora Blair
- 5 years ago
- Views:
Transcription
1 Te verpwer trip set pit i PWRs is desiged t isure te iu fuel eterlie teperature reais belw a give value T, ad te iiu rati reais abve a give value MR. Fr te give ifrati give a step by step predure, iludig all equatis, fr deteriig te trip set pit wi satisfies tese liits. Fr te purpses f tis prble, yu a assue te lat eters te re igly subled ad a steady state aalysis is valid. Itegrals wi d t ave lsed fr slutis a be left i itegral fr. Fr slutis ivlvig iterati, it is suffiiet t state wi equati(s are t be slved iteratively ad te variable(s t be iterated. Yu ay assue te fllwig ifrati is kw. Yu ay als assue ay eessary fluid ad/r terdyai prperties/relatis are available. Te eat flux prfile i te ael a be assued t be f te fr q q Z were te sape futi Z( is arbitrary but kw. Prble Paraeters Frati f Eergy epsited i Fuel Pwer Peakig Fatr Axial Peak t Average Rati Pressure Nuber f fuel rds Fuel Heigt Rd iaeter Rd Pit (square lattie Cre Ilet Etalpy Cre Mass Flux Gap Cdutae Clad Teral Cdutivity Clad Tikess Pellet iaeter f F q F P rds H S i G H G k t SOLUTION Reatr Teral Pwer Te reatr teral utput is related t te iu eat flux i te ael by Q F H q Q q H f q ffq were q q Z(. Te psiti f iu eat flux ( satisfies dz d, is idepedet f te eat flux agitude ad a be fud fr ay Z(. Give, te prble redues t fidig q tat satisfies te ad fuel teperature liits. Liit
2 Te R at ay lati witi te ael is were q q ( x (, G, P,, rit rit e e i ( xe fg f ( i q d GAx f q rit R q A S x /4 e 4[ S / 4] Te iiu R is te i[r(]. T deterie te value f = (MR TARGET, te fllwig predure a be fllwed. q wi satisfies te liit a Guess a value f q q ( q Z( b At speified ireets fr [ H /, H], pute ( x( q ( R ( ad rit e rit rit rit rit rit MR = i[r(] If MR > (MR TARGET irease q MR < (MR TARGET derease q d Retur t b ad repeat util MR = (MR TARGET q Fuel Ceterlie Liit Te fuel eterlie teperature ( T ( at ay lati is te iterative sluti f
3 69.6 Ts q R l Ts 46 T T 4 4 were te fuel surfae teperature a be writte i ters f te lad surfae teperature i te ael by R R R Ts T q l. RH i G k Ri Te vluetri eat geerati rate is related t te eat flux by q R q. ( ( Te lad teperature is a futi f te lal eat trasfer regie. Sie it is give tat te fluid eters igly subled, te pssible eat trasfer regies are sigle pase fre veti, ixed bilig ad fully develped uleate bilig. Fr a give eat flux, te first step ivlves deteriig te bilig budaries. Trasiti fr Sigle Pase Fred Cveti t Mixed ilig At te Iipiet ilig Pit (,.56 q ( q ( 5.6 P T ( T sat.34.3/ P were is te sigle-pase fred veti eat trasfer effiiet ad a be btaied fr te Weisa Crrelati.8 k Ge C p C( S / e k /3. T ( is te lal fluid teperature ad a be btaied fr te etalpy at ay lati by T T (, P, were ( i q d GAx f Fr a give ass flux, ilet ditis ad eat flux prfile, te ly ukw is, wi ay be slved fr iteratively. Trasiti fr Mixed t Fully evelped Nuleate ilig At te trasiti pit betwee ixed ad fully develped uleate bilig (
4 / q ( q ( q q q q were q ( [ T ( T ] 6 sat q ( T ( T ( q [ T T ] q ( ( sat 6 T T T T (, P Fr a give eat flux prfile ad ael peratig ditis, tese equati redue t a sigle liear equati i te bilig trasiti pit ad ay be slved iteratively T T(, P. Oe te bilig budaries are kw, te lad teperature at ay lati a be deteried. Clad Teperature istributi Give te bilig budaries, te lad teperature is Sigle Pase Fred Cveti Regi [, ] q T T Mixed ilig Regi [, ] Te wall teperature at ay lati i te ixed bilig regi is te sluti f q q ( q q q q were: q ( [ T T ] / q ( 6 [ T ] T sat
5 ad te ly ukw at ay lati is T ( wi ay be slved fr iteratively. 3 Fully evelped Nuleate ilig Regi I te Fully evelped Nuleate ilig Regi, te lad teperature a be deteried diretly fr q T Tsat 6 Predure fr deteriig te eat flux wi satisfies te fuel eterlie liit a Guess q q ( q Z( q( b Cpute te bilig budaries ad At speified ireets fr [, H] pute T (, T ( ad T ( d if [ T ( ] > T derease q s [ T ( ] < T irease q e Retur t b ad repeat util T = T q [ ( ] T Te eat flux wi satisfies bt liits is q i q, q T. Te trip set pit is te H Q TRIP q Z( F f q
A New Method for Finding an Optimal Solution. of Fully Interval Integer Transportation Problems
Applied Matheatical Scieces, Vl. 4, 200,. 37, 89-830 A New Methd fr Fidig a Optial Sluti f Fully Iterval Iteger Trasprtati Prbles P. Padia ad G. Nataraja Departet f Matheatics, Schl f Advaced Scieces,
Axial Temperature Distribution in W-Tailored Optical Fibers
Axial Temperature Distributi i W-Tailred Optical ibers Mhamed I. Shehata (m.ismail34@yah.cm), Mustafa H. Aly(drmsaly@gmail.cm) OSA Member, ad M. B. Saleh (Basheer@aast.edu) Arab Academy fr Sciece, Techlgy
Identical Particles. We would like to move from the quantum theory of hydrogen to that for the rest of the periodic table
We wuld like t ve fr the quatu thery f hydrge t that fr the rest f the peridic table Oe electr at t ultielectr ats This is cplicated by the iteracti f the electrs with each ther ad by the fact that the
Control Systems. Controllability and Observability (Chapter 6)
6.53 trl Systems trllaility ad Oservaility (hapter 6) Geeral Framewrk i State-Spae pprah Give a LTI system: x x u; y x (*) The system might e ustale r des t meet the required perfrmae spe. Hw a we imprve
MATH Midterm Examination Victor Matveev October 26, 2016
MATH 33- Midterm Examiati Victr Matveev Octber 6, 6. (5pts, mi) Suppse f(x) equals si x the iterval < x < (=), ad is a eve peridic extesi f this fucti t the rest f the real lie. Fid the csie series fr
Multi-objective Programming Approach for. Fuzzy Linear Programming Problems
Applied Mathematical Scieces Vl. 7 03. 37 8-87 HIKARI Ltd www.m-hikari.cm Multi-bective Prgrammig Apprach fr Fuzzy Liear Prgrammig Prblems P. Padia Departmet f Mathematics Schl f Advaced Scieces VIT Uiversity
Examination No. 3 - Tuesday, Nov. 15
NAME (lease rit) SOLUTIONS ECE 35 - DEVICE ELECTRONICS Fall Semester 005 Examiati N 3 - Tuesday, Nv 5 3 4 5 The time fr examiati is hr 5 mi Studets are allwed t use 3 sheets f tes Please shw yur wrk, artial
Chapter 8 Sections 8.4 through 8.6 Internal Flow: Heat Transfer Correlations. In fully-developed region. Neglect axial conduction
Chapter 8 Sectin 8.4 thrugh 8.6 Internal Flw: Heat Tranfer Crrelatin T v cu p cp ( rt) k r T T k x r r r r r x In fully-develped regin Neglect axial cnductin u ( rt) r x r r r r r x T v T T T T T u r x
Chapter 3.1: Polynomial Functions
Ntes 3.1: Ply Fucs Chapter 3.1: Plymial Fuctis I Algebra I ad Algebra II, yu ecutered sme very famus plymial fuctis. I this secti, yu will meet may ther members f the plymial family, what sets them apart
Chapter 4: Angle Modulation
57 Chapter 4: Agle Modulatio 4.1 Itrodutio to Agle Modulatio This hapter desribes frequey odulatio (FM) ad phase odulatio (PM), whih are both fors of agle odulatio. Agle odulatio has several advatages
Quantum Mechanics for Scientists and Engineers. David Miller
Quatum Mechaics fr Scietists ad Egieers David Miller Time-depedet perturbati thery Time-depedet perturbati thery Time-depedet perturbati basics Time-depedet perturbati thery Fr time-depedet prblems csider
ALE 26. Equilibria for Cell Reactions. What happens to the cell potential as the reaction proceeds over time?
Name Chem 163 Secti: Team Number: AL 26. quilibria fr Cell Reactis (Referece: 21.4 Silberberg 5 th editi) What happes t the ptetial as the reacti prceeds ver time? The Mdel: Basis fr the Nerst quati Previusly,
Chapter 9 Frequency-Domain Analysis of Dynamic Systems
ME 43 Systes Dyaics & Ctrl Chapter 9: Frequecy Dai Aalyis f Dyaic Systes Systes Chapter 9 Frequecy-Dai Aalysis f Dyaic Systes 9. INTRODUCTION A. Bazue The ter Frequecy Respse refers t the steady state
Pipe Networks - Hardy Cross Method Page 1. Pipe Networks
Pie Netwrks - Hardy Crss etd Page Pie Netwrks Itrducti A ie etwrk is a itercected set f ies likig e r mre surces t e r mre demad (delivery) its, ad ca ivlve ay umber f ies i series, bracig ies, ad arallel
HCB-3 Edition. Solutions Chapter 12 Problems. SOLUTION: Refer to saturated steam table (Table A3-SI) and superheated steam table (Table A4-SI)
HCB- Editin 12.1 Slutins Chapter 12 Prbles GIVEN: Fllwing table fr water: T (C p (kpa v ( /kg Phase 60 (1.25 (2 ( 175 (4 Saturated vapr 00 00 (5 (6 100 10 (7 (8 (9 (10 0.001097 Saturated vapr 1000 10 (11
Grade 3 Mathematics Course Syllabus Prince George s County Public Schools
Ctet Grade 3 Mathematics Curse Syllabus Price Gerge s Cuty Public Schls Prerequisites: Ne Curse Descripti: I Grade 3, istructial time shuld fcus fur critical areas: (1) develpig uderstadig f multiplicati
th th th The air-fuel ratio is determined by taking the ratio of the mass of the air to the mass of the fuel,
Cheical Reactins 14-14 rpane is burned wi 75 percent excess during a cbustin prcess. The AF rati is t be deterined. Assuptins 1 Cbustin is cplete. The cbustin prducts cntain CO, H O, O, and N nly. rperties
DETERMINATION OF NATURAL FREQUENCY AND DAMPING RATIO
Hasa G Pasha DETERMINATION OF NATURAL FREQUENCY AND DAMPING RATIO OBJECTIVE Deterie the atural frequecy ad dapig ratio for a aluiu catilever bea, Calculate the aalytical value of the atural frequecy ad
cannot commute.) this idea, we can claim that the average value of the energy is the sum of such terms over all points in space:
Che 441 Quatu Cheistry Ntes May, 3 rev VI. Apprxiate Slutis A. Variati Methd ad Huckel Mlecular Orbital (HMO) Calculatis Refereces: Liberles, Ch. 4, Atkis, Ch. 8, Paulig ad Wils Streitweiser, "MO Thery
Solutions. Definitions pertaining to solutions
Slutis Defiitis pertaiig t slutis Slute is the substace that is disslved. It is usually preset i the smaller amut. Slvet is the substace that des the disslvig. It is usually preset i the larger amut. Slubility
e) Dates of Violation(S) reference ( page of report /data sheet): March 25, 2010, page 2
e) tes f Vilti(S) referee ( pge f reprt /dt sheet): Mrh 25, 2, pge 2 ) Explti f use(s): gig trtrs wrkig rretig plt defiieies, d trubleshtig filter prbles. g) rretie ti(s): trtrs d P re wrkig t rret prbles
Daniel López Gaxiola 1 Student View Jason M. Keith
Suppleental Material for Transport Process and Separation Process Principles Chapter Principles of Moentu Transfer and Overall Balances In fuel cells, the fuel is usually in gas or liquid phase. Thus,
Every gas consists of a large number of small particles called molecules moving with very high velocities in all possible directions.
Kietic thery f gases ( Kietic thery was develped by Berlli, Jle, Clasis, axwell ad Bltzma etc. ad represets dyamic particle r micrscpic mdel fr differet gases sice it thrws light the behir f the particles
rcrit (r C + t m ) 2 ] crit + t o crit The critical radius is evaluated at a given axial location z from the equation + (1 , and D = 4D = 555.
![rcrit (r C + t m ) 2 ] crit + t o crit The critical radius is evaluated at a given axial location z from the equation + (1 , and D = 4D = 555.](/thumbs/71/66154865.jpg "rcrit (r C + t m ) 2 ] crit + t o crit The critical radius is evaluated at a given axial location z from the equation + (1 , and D = 4D = 555.")
hapter 1 c) When the average bld velcity in the capillary is reduced by a factr f 10, the delivery f the slute t the capillary is liited s that the slute cncentratin after crit 0.018 c is equal t er at
NAME Borough of Manhattan Community College Course Physics 110 Sec 721 Instructor: Dr. Hulan E. Jack Jr. Date December 19, 2006
Brug f Manattan unity llege urse Pysics 110 Sec 721 nstructr: Dr. Hulan E. Jack Jr. Date Deceber 19, 2006 inal Exa NSTRUTONS - D 7 prbles : D Prble 1, 2 fr Prble 2,3 and 4, 2 fr Prbles 5,6 and 7, 2 fr
E o and the equilibrium constant, K
lectrchemical measuremets (Ch -5 t 6). T state the relati betwee ad K. (D x -b, -). Frm galvaic cell vltage measuremet (a) K sp (D xercise -8, -) (b) K sp ad γ (D xercise -9) (c) K a (D xercise -G, -6)
(s)h(s) = K( s + 8 ) = 5 and one finite zero is located at z 1
ROOT LOCUS TECHNIQUE 93 should be desiged differetly to eet differet specificatios depedig o its area of applicatio. We have observed i Sectio 6.4 of Chapter 6, how the variatio of a sigle paraeter like
The Excel FFT Function v1.1 P. T. Debevec February 12, The discrete Fourier transform may be used to identify periodic structures in time ht.
The Excel FFT Fucti v P T Debevec February 2, 26 The discrete Furier trasfrm may be used t idetify peridic structures i time ht series data Suppse that a physical prcess is represeted by the fucti f time,
Sound Absorption Characteristics of Membrane- Based Sound Absorbers
Purdue e-pubs Publicatis f the Ray W. Schl f Mechaical Egieerig 8-28-2003 Sud Absrpti Characteristics f Membrae- Based Sud Absrbers J Stuart Blt, blt@purdue.edu Jih Sg Fllw this ad additial wrks at: http://dcs.lib.purdue.edu/herrick
Electrostatics. . where,.(1.1) Maxwell Eqn. Total Charge. Two point charges r 12 distance apart in space
Maxwell Eq. E ρ Electrstatics e. where,.(.) first term is the permittivity i vacuum 8.854x0 C /Nm secd term is electrical field stregth, frce/charge, v/m r N/C third term is the charge desity, C/m 3 E
Markov processes and the Kolmogorov equations
Chapter 6 Markv prcesses ad the Klmgrv equatis 6. Stchastic Differetial Equatis Csider the stchastic differetial equati: dx(t) =a(t X(t)) dt + (t X(t)) db(t): (SDE) Here a(t x) ad (t x) are give fuctis,
Homework (Kittel 7.1) Density of orbitals in one and two dimensions.
Hoework 8.. Kittel 7. esity of orbitals i oe a two iesios. a Sow tat te esity of orbitals of a free eletro i oe iesio is were is te legt of te lie. b. Sow tat i two iesios, for a square of area, iepeet
Digital Signal Processing. Homework 2 Solution. Due Monday 4 October Following the method on page 38, the difference equation
Digital Sigal Proessig Homework Solutio Due Moda 4 Otober 00. Problem.4 Followig the method o page, the differee equatio [] (/4[-] + (/[-] x[-] has oeffiiets a0, a -/4, a /, ad b. For these oeffiiets A(z
Modeling Micromixing Effects in a CSTR
delig irixig Effes i a STR STR, f all well behaved rears, has he wides RTD i.e. This eas ha large differees i perfrae a exis bewee segregaed flw ad perais a axiu ixedess diis. The easies hig rea is he
Chapter 5: Properties of Solutions
hapter 5: rperties Slutis 1. Wax is a slid ixture hydrcar cpuds csistig lecules with lg chais car ats. Which slvet wuld yu expect t e st capale disslvig wax? N-plar will disslve i plar slvet a. HOH. H
First-Principles Modelling of Electrospraying, and the Effects of Dissipation in Electrospray Thrusters
First-Priciples Mdellig f Electrsprayig, ad the Effects f Dissipati i Electrspray Thrusters IEPC-7-49 Preseted at the 35th Iteratial Electric Prpulsi Cferece Gergia Istitute f Techlgy Atlata, Gergia USA
The state space model needs 5 parameters, so it is not as convenient to use in this control study.
Trasfer fuctio for of the odel G θ K ω 2 θ / v θ / v ( s) = = 2 2 vi s + 2ζωs + ω The followig slides detail a derivatio of this aalog eter odel both as state space odel ad trasfer fuctio (TF) as show
Turbulent entry length. 7.3 Turbulent pipe flow. Turbulent entry length. Illustrative experiment. The Reynolds analogy and heat transfer
Turulet etry legt 7.3 Turulet ie l Etry legts x e ad x et are geerally srter turulet l ta lamar l Termal etry legts, x et /, r a case it q cst imsed a ydrdyamically ully develed l 7.3 Turulet ie l ill
Solutions to Midterm II. of the following equation consistent with the boundary condition stated u. y u x y
Sltis t Midterm II Prblem : (pts) Fid the mst geeral slti ( f the fllwig eqati csistet with the bdary cditi stated y 3 y the lie y () Slti : Sice the system () is liear the slti is give as a sperpsiti
Study of Energy Eigenvalues of Three Dimensional. Quantum Wires with Variable Cross Section
Adv. Studies Ther. Phys. Vl. 3 009. 5 3-0 Study f Eergy Eigevalues f Three Dimesial Quatum Wires with Variale Crss Secti M.. Sltai Erde Msa Departmet f physics Islamic Aad Uiversity Share-ey rach Ira alrevahidi@yah.cm
Lecture 10: Bounded Linear Operators and Orthogonality in Hilbert Spaces
Lecture : Bouded Liear Operators ad Orthogoality i Hilbert Spaces 34 Bouded Liear Operator Let ( X, ), ( Y, ) i i be ored liear vector spaces ad { } X Y The, T is said to be bouded if a real uber c such
University of Washington Department of Chemistry Chemistry 453 Winter Quarter 2015
Uiversity of Wasigto Departmet of Cemistry Cemistry 453 Witer Quarter 15 Lecture 14. /11/15 Recommeded Text Readig: Atkis DePaula: 9.1, 9., 9.3 A. Te Equipartitio Priciple & Eergy Quatizatio Te Equipartio
Keywords : Distributed Load, Non-uniform, Elastic Foundation, moving Mass. GJSFR-F Classication : FOR Code:
Glbal Jural Sciece Frtier Research Matheatics & Decisi Scieces Vlue 1 Issue 3 Versi 1. March 1 Type : Duble Blid Peer Reviewed Iteratial Research Jural Publisher: Glbal Jurals Ic. (USA Olie ISSN: 49-466
Partial Differential Equations
EE 84 Matematical Metods i Egieerig Partial Differetial Eqatios Followig are some classical partial differetial eqatios were is assmed to be a fctio of two or more variables t (time) ad y (spatial coordiates).
School of Mechanical Engineering Purdue University. ME375 Transfer Functions - 1
Trasfer Fuctio Aalysis Free & Forced Resposes Trasfer Fuctio Syste Stability ME375 Trasfer Fuctios - 1 Free & Forced Resposes Ex: Let s look at a stable first order syste: y y Ku Take LT of the I/O odel
are specified , are linearly independent Otherwise, they are linearly dependent, and one is expressed by a linear combination of the others
Chater 3. Higher Order Liear ODEs Kreyszig by YHLee;4; 3-3. Hmgeeus Liear ODEs The stadard frm f the th rder liear ODE ( ) ( ) = : hmgeeus if r( ) = y y y y r Hmgeeus Liear ODE: Suersiti Pricile, Geeral
6-5. H 2 O 200 kpa 200 C Q. Entropy Changes of Pure Substances
Canges f ure Substances 6-0C Yes, because an ternally reversible, adiabatic prcess vlves n irreversibilities r eat transfer. 6- e radiatr f a steam eatg system is itially filled wit supereated steam. e
u = A Z Chemistry 110 Fall 2010 Rayleigh-Jeans Law for Blackbody SI Units SI Units Secondary Units written in terms of Primary
SI Uits Key Study Pits fr Petrucci et al., Secdary Uits writte i terms f Primary Capters 8 & 9 Nte: Fudametal cstats ad a peridic table will be prvided te midterm but equatis will t be give. Cemistry 0
Vasyl Moisyshyn*, Bogdan Borysevych*, Oleg Vytyaz*, Yuriy Gavryliv*
AGH DRILLING, OIL, GAS Vol. 3 No. 3 204 http://dx.doi.org/0.7494/drill.204.3.3.43 Vasyl Moisyshy*, Bogda Borysevych*, Oleg Vytyaz*, Yuriy Gavryliv* DEVELOPMENT OF THE MATHEMATICAL MODELS OF THE INTEGRAL
Exergoeconomic Analysis of Two-stage Thermoelectric Cooler with Genetic Algorithm Sudhanshu Sharma a,*, V. K. Dwivedi b, S. N.
Vlue 4, Issue 1(016) 4-8 ISSN 347-358 Iteratial Jural f Advae Resear ad Ivati Exergei Aalysis f -stage ereletri Cler it Geeti Algrit Sudasu Sara a,*, V. K. Divedi b, S. N. Padit a Deartet f Meaial Egieerig,
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
The maximum heat transfer rate is for an infinite area counter flow heat exchanger.
IAM Heat Exangers 9. Aendix Illustratin f se nets in eat exangers 9.. Heat Exanger Effetiveness is is defined as: Atual Heat ransfer ate Maxiu Pssible Heat ransfer ate q q ax e axiu eat transfer rate is
Fourier Method for Solving Transportation. Problems with Mixed Constraints
It. J. Ctemp. Math. Scieces, Vl. 5, 200,. 28, 385-395 Furier Methd fr Slvig Trasprtati Prblems with Mixed Cstraits P. Padia ad G. Nataraja Departmet f Mathematics, Schl f Advaced Scieces V I T Uiversity,
Heat exchanger. Heat exchanger
s are deves n w eat s transferred between tw fluds at dfferent teperatures wtut any xng f fluds. type. Dret eat transfer type 2. Strage type 3. Dret ntat type ttps://www.faebk./0000085304058/vdes/96230780490756/.
Chapter 2. Asymptotic Notation
Asyptotic Notatio 3 Chapter Asyptotic Notatio Goal : To siplify the aalysis of ruig tie by gettig rid of details which ay be affected by specific ipleetatio ad hardware. [1] The Big Oh (O-Notatio) : It
A Simplified Nonlinear Generalized Maxwell Model for Predicting the Time Dependent Behavior of Viscoelastic Materials
Wrld Jural f Mechaics, 20,, 58-67 di:0.4236/wj.20.302 Published Olie Jue 20 (http://www.scirp.rg/jural/wj) A Siplified Nliear Geeralized Maxwell Mdel fr Predictig the Tie Depedet Behavir f Viscelastic
REVERSIBLE NON-FLOW PROCESS CONSTANT VOLUME PROCESS (ISOCHORIC PROCESS) In a constant volume process, he working substance is contained in a rigid
REVERSIBLE NON-FLOW PROCESS CONSTANT VOLUME PROCESS (ISOCHORIC PROCESS) I a ostat olume roess, he workig substae is otaied i a rigid essel, hee the boudaries of the system are immoable, so work aot be
Mechanical Vibrations
Mechaical Vibratios Cotets Itroductio Free Vibratios o Particles. Siple Haroic Motio Siple Pedulu (Approxiate Solutio) Siple Pedulu (Exact Solutio) Saple Proble 9. Free Vibratios o Rigid Bodies Saple Proble
Dynamic Response of Second Order Mechanical Systems with Viscous Dissipation forces
Hadut #a (pp. 1-39) Dyamic Respse f Secd Order Mechaical Systems with Viscus Dissipati frces d X d X + + = ext() t M D K X F dt dt Free Respse t iitial cditis ad F (t) = 0, Uderdamped, Critically Damped
A Hartree-Fock Calculation of the Water Molecule
Chemistry 460 Fall 2017 Dr. Jea M. Stadard Nvember 29, 2017 A Hartree-Fck Calculati f the Water Mlecule Itrducti A example Hartree-Fck calculati f the water mlecule will be preseted. I this case, the water
Main components of the above cycle are: 1) Boiler (steam generator) heat exchanger 2) Turbine generates work 3) Condenser heat exchanger 4) Pump
Introducton to Terodynacs, Lecture -5 Pro. G. Cccarell (0 Applcaton o Control olue Energy Analyss Most terodynac devces consst o a seres o coponents operatng n a cycle, e.g., stea power plant Man coponents
Transfer Function Analysis
Trasfer Fuctio Aalysis Free & Forced Resposes Trasfer Fuctio Syste Stability ME375 Trasfer Fuctios - Free & Forced Resposes Ex: Let s s look at a stable first order syste: τ y + y = Ku Take LT of the I/O
Lecture 18. MSMPR Crystallization Model
ecture 18. MSMPR Crystalliati Mdel MSMPR Crystalliati Mdel Crystal-Ppulati alace - Number f crystals - Cumulative umber f crystals - Predmiat crystal sie - Grwth rate MSMPR Crystalliati Mdel Mixed-suspesi,
REDUCING THE POSSIBILITY OF SUBJECTIVE ERROR IN THE DETERMINATION OF THE STRUCTURE-FUNCTION-BASED EFFECTIVE THERMAL CONDUCTIVITY OF BOARDS
Nice, Côte d Azur, Frace, 27-29 Septeber 2006 REDUCING THE POSSIBILITY OF SUBJECTIVE ERROR IN THE DETERMINATION OF THE STRUCTURE-FUNCTION-BASED EFFECTIVE THERMAL CONDUCTIVITY OF BOARDS Erő Kollár, Vladiír
Earlier Lecture. This gas tube is called as Pulse Tube and this phenomenon is called as Pulse Tube action.
31 1 Earlier Leture In te earlier leture, we ave seen a Pulse Tube (PT) ryoooler in wi te meanial displaer is removed and an osillating gas flow in te tin walled tube produes ooling. Tis gas tube is alled
Chapter 3. Problem Solutions
Capter. Proble Solutions. A poton and a partile ave te sae wavelengt. Can anyting be said about ow teir linear oenta opare? About ow te poton's energy opares wit te partile's total energy? About ow te
STRUCTURES IN MIKE 21. Flow over sluice gates A-1
A-1 STRUCTURES IN MIKE 1 Fl ver luice gate Fr a give gemetry f the luice gate ad k ater level uptream ad dtream f the tructure, the fl rate, ca be determied thrugh the equati f eergy ad mmetum - ee B Pedere,
S. A. ALIEV, Y. I. YELEYKO, Y. V. ZHERNOVYI. STEADY-STATE DISTRIBUTIONS FOR CERTAIN MODIFICATIONS OF THE M/M/1/m QUEUEING SYSTEM
Trasactios of Azerbaija Natioal Acadey of Scieces, Series of Physical-Techical ad Matheatical Scieces: Iforatics ad Cotrol Probles 009 Vol XXIX, 6 P 50-58 S A ALIEV, Y I YELEYKO, Y V ZHERNOVYI STEADY-STATE
(b) The heat transfer can be determined from an energy balance on the system
8-5 Heat is transferred to a iston-cylinder device wit a set of stos. e work done, te eat transfer, te exergy destroyed, and te second-law efficiency are to be deterined. Assutions e device is stationary
/ / MET Day 000 NC1^ INRTL MNVR I E E PRE SLEEP K PRE SLEEP R E
05//0 5:26:04 09/6/0 (259) 6 7 8 9 20 2 22 2 09/7 0 02 0 000/00 0 02 0 04 05 06 07 08 09 0 2 ay 000 ^ 0 X Y / / / / ( %/ ) 2 /0 2 ( ) ^ 4 / Y/ 2 4 5 6 7 8 9 2 X ^ X % 2 // 09/7/0 (260) ay 000 02 05//0
Chapter 1 Electrons, Bonds and Molecular Properties
hapter 1 Electrons, Bonds and Molecular Properties Review of oncepts Fill in the blanks below. To verify that your answers are correct, look in your textbook at the end of hapter 1. Each of the sentences
Unit -2 THEORY OF DILUTE SOLUTIONS
Uit - THEORY OF DILUTE SOLUTIONS 1) hat is sluti? : It is a hmgeus mixture f tw r mre cmpuds. ) hat is dilute sluti? : It is a sluti i which slute ccetrati is very less. 3) Give a example fr slid- slid
SEQUENTIAL ESTIMATION IN A SUBCLASS OF EXPONENTIAL FAMILY UNDER WEIGHTED SQUARED ERROR LOSS *
Iraia Jural f iee & Tehlgy Trasati A Vl.. A Prited i The Islami Republi f Ira 007 hiraz Uiersity QUTIAL TIMATIO I A UBCLA OF POTIAL FAMIL UDR WIGHTD QUARD RROR LO *. MATOLLAHI ** M. JAFARI JOZAI AD. MAHLOOJI
Fluids Lecture 2 Notes
Fluids Leture Notes. Airfoil orte Sheet Models. Thi-Airfoil Aalysis Problem Readig: Aderso.,.7 Airfoil orte Sheet Models Surfae orte Sheet Model A aurate meas of represetig the flow about a airfoil i a
Exercises for Frequency Response. ECE 102, Winter 2011, F. Najmabadi
Eercses r Frequency espnse EE 0, Wnter 0, F. Najabad Eercse : A Mdy the crcut belw t nclude a dnant ple at 00 Mz ( 00 Ω, k, k, / 00 Ω, λ 0, and nre nternal capactances the MOS. pute the dnant ple n the
Application of Homotopy Analysis Method for Solving various types of Problems of Ordinary Differential Equations
Iteratioal Joural o Recet ad Iovatio Treds i Coputig ad Couicatio IN: 31-8169 Volue: 5 Issue: 5 16 Applicatio of Hootopy Aalysis Meod for olvig various types of Probles of Ordiary Differetial Equatios
Observer Design with Reduced Measurement Information
Observer Desig with Redued Measuremet Iformatio I pratie all the states aot be measured so that SVF aot be used Istead oly a redued set of measuremets give by y = x + Du p is available where y( R We assume
x 2 x 3 x b 0, then a, b, c log x 1 log z log x log y 1 logb log a dy 4. dx As tangent is perpendicular to the x axis, slope
The agle betwee the tagets draw t the parabla y = frm the pit (-,) 5 9 6 Here give pit lies the directri, hece the agle betwee the tagets frm that pit right agle Ratig :EASY The umber f values f c such
DYNAMICS VECTOR MECHANICS FOR ENGINEERS: Mechanical Vibrations. Seventh Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr.
Seveth Editio CHAPTER 9 VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Ferdiad P. Beer E. Russell Johsto, Jr. Mechaical Vibratios Lecture Notes: J. Walt Oler Texas Tech Uiversity 003 The McGraw-Hill Copaies,
ACTIVE FILTERS EXPERIMENT 2 (EXPERIMENTAL)
EXPERIMENT ATIVE FILTERS (EXPERIMENTAL) OBJETIVE T desig secd-rder lw pass ilters usig the Salle & Key (iite psitive- gai) ad iiite-gai apliier dels. Oe circuit will exhibit a Butterwrth respse ad the
Absorption and Emission of Radiation: Time Dependent Perturbation Theory Treatment
Absorptio ad Eissio of Radiatio: Tie Depedet Perturbatio Theory Treatet Wat Hailtoia for Charged Partile i E & M Field Need the potetial U. Fore o Charged Partile: 1 F e E V B Fore (geeralized for i Lagragia
Chapter 4. Problem Solutions
Chapter 4. Prblem Slutis. The great majrity f alpha particles pass thrugh gases ad thi metal fils with deflectis. T what cclusi abut atmic structure des this bservati lead? The fact that mst particles
Computational Methods CMSC/AMSC/MAPL 460. Quadrature: Integration
Computatioal Metods CMSC/AMSC/MAPL 6 Quadrature: Itegratio Ramai Duraiswami, Dept. o Computer Siee Some material adapted rom te olie slides o Eri Sadt ad Diae O Leary Numerial Itegratio Idea is to do itegral
Lecture 3 Heat Exchangers
L3 Leture 3 Heat Exangers Heat Exangers. Heat Exangers Transfer eat from one fluid to anoter. Want to imise neessary ardware. Examples: boilers, ondensors, ar radiator, air-onditioning oils, uman body.
WEST VIRGINIA UNIVERSITY
WEST VIRGINIA UNIVERSITY PLASMA PHYSICS GROUP INTERNAL REPORT PL - 045 Mea Optical epth ad Optical Escape Factr fr Helium Trasitis i Helic Plasmas R.F. Bivi Nvember 000 Revised March 00 TABLE OF CONTENT.0
Module 7: Solved Problems
Mdule 7: Slved Prblems 1 A tn-walled nentr tube eat exanger f 019-m lengt s t be used t eat denzed water frm 40 t 60 at a flw rate f 5 kg/s te denzed water flws trug te nner tube f 30-mm dameter wle t
General Amplifiers. Analog Electronics Circuits Nagamani A N. Lecturer, PESIT, Bangalore 85. Cascade connection - FET & BJT
Analg lectrnics Circuits Nagamani A N Lecturer, PST, Bangalre 85 mail nagamani@pes.edu General Amplifiers Cascade cnnectin - FT & BJT Numerical Cascde cnnectin arlingtn cnnectin Packaged arlingtn cnnectin
Ch. 1 Introduction to Estimation 1/15
Ch. Itrducti t stimati /5 ample stimati Prblem: DSB R S f M f s f f f ; f, φ m tcsπf t + φ t f lectrics dds ise wt usually white BPF & mp t s t + w t st. lg. f & φ X udi mp cs π f + φ t Oscillatr w/ f
11. Ideal Gas Mixture
. Ideal Ga xture. Geeral oderato ad xture of Ideal Gae For a geeral xture of N opoet, ea a pure ubtae [kg ] te a for ea opoet. [kol ] te uber of ole for ea opoet. e al a ( ) [kg ] N e al uber of ole (
Conventional propellers in CRP-POD configuration. Tests and extrapolation.
ifth Iteratial ypsiu Marie Prpulsrs MP 17, Esp, ilad, ue 017 vetial prpellers i P-PO cfigurati. ests ad extraplati. aó uereda 1, Maria Pérez-bri, ua Gzález-Adalid, ristia ria 1 1 Ita-ehipar, aal de Experiecias
An object is placed 20 cm in front of a convex mirror that has a radius of curvature of magnitude 16 cm (note this is not the focal length).
A bjet is plae 0 m i frt f a ex mirrr that has a raius f urature f magitue 6 m (te this is t the fal legth). ) Desribe the image frme: a) real a ierte b) real a upright ) irtual a ierte ) irtual a upright
Chemistry 432 Problem Set 11 Spring 2018 Solutions
1. Show that for an ideal gas Cheistry 432 Proble Set 11 Spring 2018 Solutions P V 2 3 < KE > where is the average kinetic energy of the gas olecules. P 1 3 ρ v2 KE 1 2 v2 ρ N V P V 1 3 N v2 2 3 N
MATHEMATICS 9740/01 Paper 1 14 Sep hours
Cadidate Name: Class: JC PRELIMINARY EXAM Higher MATHEMATICS 9740/0 Paper 4 Sep 06 3 hurs Additial Materials: Cver page Aswer papers List f Frmulae (MF5) READ THESE INSTRUCTIONS FIRST Write yur full ame
Data Sheet. ACPL-8x7 Multi-Channel Full-Pitch Phototransistor Optocoupler. Description. Features. ACPL-827 pin layout.
ACPL-8x7 Multi-Channel ull-pitch Phttransistr Optcupler Data Sheet Lead (Pb) ree RHS 6 fully cmpliant RHS 6 fully cmpliant ptins available; -xxxe dentes a lead-free prduct Descriptin The ACPL-827 is a
FILE NAME I:\120183\Elec\120183_E-119.dwg SAVED ON 1/28/2013 2:04 PM PLOTTED ON 1/28/2013 2:04 PM PLOTTED BY HUANG, TINGEN
ARHTETURE EGEERG TERR DESG SHELT, ETUT HARTFRD, ETUT SMERSET, EW JERSEY EW YRK, EW YRK APLES, FLRDA ST, MASSAHUSETTS 617-524 - 5200 SULTAT: THS DRAWG AD DETAL T, AS A STRUMET F SERVE, S THE PRPERTY F FLETHER
INDEPENDENT COMPONENT ANALYSIS USING JAYNES MAXIMUM ENTROPY PRINCIPLE. Deniz Erdogmus, Kenneth E. Hild II, Yadunandana N. Rao, Jose C.
IDEPEDE COMPOE AALYSIS USIG JAYES MAXIMUM EROPY PRICIPLE Deiz Erdgus, Keeth E. Hild II, Yaduadaa. Ra, Jse C. Pricipe CEL, ECE Departet, Uiversity f Flrida, Gaiesville, FL 326, USA ABSRAC ICA deals with
[1 & α(t & T 1. ' ρ 1
NAME 89.304 - IGNEOUS & METAMORPHIC PETROLOGY DENSITY & VISCOSITY OF MAGMAS I. Desity The desity (mass/vlume) f a magma is a imprtat parameter which plays a rle i a umber f aspects f magma behavir ad evluti.
6.867 Machine learning, lecture 14 (Jaakkola)
6.867 Machie learig, lecture 14 (Jaakkla) 1 Lecture tpics: argi ad geeralizati liear classifiers esebles iture dels Margi ad geeralizati: liear classifiers As we icrease the uber f data pits, ay set f
Sinusoidal Steady-state Analysis
Siusoidal Steady-state Aalysis Complex umber reviews Phasors ad ordiary differetial equatios Complete respose ad siusoidal steady-state respose Cocepts of impedace ad admittace Siusoidal steady-state aalysis
Lecture 19. Curve fitting I. 1 Introduction. 2 Fitting a constant to measured data
Lecture 9 Curve fittig I Itroductio Suppose we are preseted with eight poits of easured data (x i, y j ). As show i Fig. o the left, we could represet the uderlyig fuctio of which these data are saples