SAFE OPERATION OF TUBULAR (PFR) ADIABATIC REACTORS. FIGURE 1: Temperature as a function of space time in an adiabatic PFR with exothermic reaction.

Similar documents
ENGG 1203 Tutorial. Difference Equations. Find the Pole(s) Finding Equations and Poles

Some Families of Higher Order Three-Step Iterative Techniques. where is a real number and y (5)

ENGO 431 Analytical Photogrammetry

GUC (Dr. Hany Hammad) 4/20/2016

ChE 471 Lecture 10 Fall 2005 SAFE OPERATION OF TUBULAR (PFR) ADIABATIC REACTORS

Chapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series

m = Mass flow rate The Lonely Electron Example 0a:

Electrical field generated by a charged harmonic oscillator at thermodynamic equilibrium

Handout 32. Electronic Energy Transport and Thermoelectric Effects

On Jackson's Theorem

The angle between L and the z-axis is found from

ELEC9721: Digital Signal Processing Theory and Applications

Handout 30. Optical Processes in Solids and the Dielectric Constant

Galaxy Photometry. Recalling the relationship between flux and luminosity, Flux = brightness becomes

ADDITIVE INTEGRAL FUNCTIONS IN VALUED FIELDS. Ghiocel Groza*, S. M. Ali Khan** 1. Introduction

MATH Midterm Examination Victor Matveev October 26, 2016

Axe Wo. Blood Circle Just like with using knives, when we are using an axe we have to keep an area around us clear. Axe Safety Check list:

Propagation of Light About Rapidly Rotating Neutron Stars. Sheldon Campbell University of Alberta

Helping you learn to save. Pigby s tips and tricks

Great Idea #4: Parallelism. CS 61C: Great Ideas in Computer Architecture. Pipelining Hazards. Agenda. Review of Last Lecture

Estimation of a Random Variable

2011 HSC Mathematics Extension 1 Solutions

, University. 1and. y T. since. g g

Chapter 5: Quantization of Radiation in Cavities and Free Space

Markov processes and the Kolmogorov equations

Chapter 8: Propagating Quantum States of Radiation

are specified , are linearly independent Otherwise, they are linearly dependent, and one is expressed by a linear combination of the others

GUC (Dr. Hany Hammad)

Central County Fire & Rescue - Station #5

Emigration The movement of individuals out of an area The population decreases

r ADD. TEMP. WORKSPACE

Collisionless Hall-MHD Modeling Near a Magnetic Null. D. J. Strozzi J. J. Ramos MIT Plasma Science and Fusion Center

Integrated Optical Waveguides

PREPARATORY MATHEMATICS FOR ENGINEERS

ln x = n e = 20 (nearest integer)

Chapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is

Chapter 11: Matter-Photon Interactions and Cavity Quantum Electrodynamics

CDS 101: Lecture 5.1 Reachability and State Space Feedback

Physics 111. Lecture 38 (Walker: ) Phase Change Latent Heat. May 6, The Three Basic Phases of Matter. Solid Liquid Gas

Bohr type models of the atom give a totally incorrect picture of the atom and are of only historical significance.

Chapter Five. More Dimensions. is simply the set of all ordered n-tuples of real numbers x = ( x 1

( ) ( ) ( ) 2011 HSC Mathematics Solutions ( 6) ( ) ( ) ( ) π π. αβ = = 2. α β αβ. Question 1. (iii) 1 1 β + (a) (4 sig. fig.

Lecture 20. Transmission Lines: The Basics

Mid Year Examination F.4 Mathematics Module 1 (Calculus & Statistics) Suggested Solutions

1985 AP Calculus BC: Section I

PESIT Bangalore South Campus Hosur road, 1km before Electronic City, Bengaluru -100 Department of Basic Science and Humanities

Analysis and Design of Basic Interconnects (Part 1)

ARC Window System. General Information: Determine your window type and turn to the specific pages for the. Type #1 Arc. Windows. Type #2 Arc Windows

+ x. x 2x. 12. dx. 24. dx + 1)

Trade Patterns, Production networks, and Trade and employment in the Asia-US region

Basic Interconnects at High Frequencies (Part 1)

Ch. 6 Free Electron Fermi Gas

Lecture 14. Time Harmonic Fields

Equation Sheet Please tear off this page and keep it with you

Probability & Statistics,

Q Q N, V, e, Quantum Statistics for Ideal Gas. The Canonical Ensemble 10/12/2009. Physics 4362, Lecture #19. Dr. Peter Kroll

E F. and H v. or A r and F r are dual of each other.

Option 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges.

Quantum Mechanics for Scientists and Engineers. David Miller

and the ANAVETS Unit Portage Ave, Winnipeg, Manitoba, Canada May 23 to May E L IBSF

Dielectric Waveguide 1

PURE MATHEMATICS A-LEVEL PAPER 1

Rapid growth in enrolment within the French Immersion program

UNIVERSITY OF TECHNOLOGY. Department of Mathematics PROBABILITY THEORY, STATISTICS AND OPERATIONS RESEARCH GROUP. Memorandum COSOR 76-10

The Hydrogen Atom. Chapter 7

The Real Hydrogen Atom

(, ) which is a positively sloping curve showing (Y,r) for which the money market is in equilibrium. The P = (1.4)

Narayana IIT Academy

School of Electrical Engineering. Lecture 2: Wire Antennas

Chapter 3.1: Polynomial Functions

Helping every little saver

Keywords: Auxiliary variable, Bias, Exponential estimator, Mean Squared Error, Precision.

Outline. Heat Exchangers. Heat Exchangers. Compact Heat Exchangers. Compact Heat Exchangers II. Heat Exchangers April 18, ME 375 Heat Transfer 1

Solutions. Definitions pertaining to solutions

Example

ALE 26. Equilibria for Cell Reactions. What happens to the cell potential as the reaction proceeds over time?

Chapter (8) Estimation and Confedence Intervals Examples

MONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx

ME 3600 Control Systems Frequency Domain Analysis

National Survey of Student Engagement, Spring 2011 The University at Albany, SUNY

In the name of Allah Proton Electromagnetic Form Factors

While flying from hot to cold, or high to low, watch out below!

Study of the Balance for the DHS Distribution

Assessing Student Work MATH RUBRIC. Understanding Reasoning Accuracy Communication

Multiple Short Term Infusion Homework # 5 PHA 5127

Sundials and Linear Algebra

Today s topic 2 = Setting up the Hydrogen Atom problem. Schematic of Hydrogen Atom

Outline of the Three Multiprocessor Servers from the 2009 Sun Microsystems Grant

CS 326e F2002 Lab 1. Basic Network Setup & Ethereal Time: 2 hrs

CDS 101: Lecture 5.1 Reachability and State Space Feedback

Hº = -690 kj/mol for ionization of n-propylene Hº = -757 kj/mol for ionization of isopropylene

Lecture 18. MSMPR Crystallization Model

ESCI 341 Atmospheric Thermodynamics Lesson 16 Pseudoadiabatic Processes Dr. DeCaria

Topic 5: Discrete-Time Fourier Transform (DTFT)

Statics. Consider the free body diagram of link i, which is connected to link i-1 and link i+1 by joint i and joint i-1, respectively. = r r r.

Chapter 2 Linear Waveshaping: High-pass Circuits

CHAPTER IV RESULTS. Grade One Test Results. The first graders took two different sets of pretests and posttests, one at the first

Heat/Di usion Equation. 2 = 0 k constant w(x; 0) = '(x) initial condition. ( w2 2 ) t (kww x ) x + k(w x ) 2 dx. (w x ) 2 dx 0.

Electrostatics. . where,.(1.1) Maxwell Eqn. Total Charge. Two point charges r 12 distance apart in space

Q Q N, V, e, Quantum Statistics for Ideal Gas and Black Body Radiation. The Canonical Ensemble

Transcription:

he 47 Lctu Fall 5 SFE OPERION OF UBULR (PFR DIBI REORS I a xthmic acti th tmatu will ctiu t is as mvs alg a lug flw act util all f th limitig actat is xhaust. Schmatically th aiabatic tmatu is as a fucti f sac tim, masu fm th act tac, taks th fm shw i Figu. a if FIGURE : matu as a fucti f sac tim i a aiabatic PFR with xthmic acti. h fial aiabatic tmatu a : a ( Δ H + ρ [ + β ] ( is ft xcssiv f highly xthmic systms ( β lag a s t b avi. I such situatis th l ul f thumb suggsts that w shul at i such a way that th iflcti it, i.. th it f maximum tmatu is, is v ach. his imlis that max w at with < wh is th valu f sac tim at which th iflcti it ccus.

he 47 Lctu Fall 5 Lt us w vl a cvit a siml fmula f us by acticig gis which wul guaat saf ati. si a -th ivsibl acti: R k R ( x ( t aiabatic citis tmatu a cvsi a lat by th aiabatic li quati ( + β x (3 If w fi, as i th cas f wall cl acts, th imsilss tmatu by γ (4 th cvsi i Eq. (3 ca b xss i tms f imsilss tmatu as: wh with x (5 β γ (6 γ E R (7 h at f acti valuat at aiabatic citis i tms f imsilss tmatu is btai by usig th aiabatic li q (5 t lac cvsi. h sult is: ( ( R ( γ + γ R a wh th at valuat at th f citi is: E R ( R k (8 (9 h gy balac f aiabatic PFR ati is: ( Δ H ( R a ρ ( Witt i tms f imsilss tmatu it bcms:

he 47 Lctu Fall 5 R γ ( γ + wh th chaactistic acti tim is: ( R ( R ( h iitial citi is (3 W ca wit Eq. ( i th mst cmact way by fiig th Damkhl umb as th ati f chaactistic css tim a acti tim, i.. Da ( R (4 R Equati ( a iitial citi (3 bcm: ( Da γ ( γ + (5 t Da (6 Nw w wat t hav th act sht ugh (limit th cvsi achivabl s that w ca k th iflcti it ut f th act i.. w t lt it ccu i th act. h citical tmatu at iflcti it, if, is btai by sttig ( Da (7 which sults i a quati f if yilig: [ γ + 4 ( γ + γ ]; γ if (8a, (8b if 3

he 47 Lctu Fall 5 h sult f th zth acti, q (8b, ca b btai by alyig th L Hsital ul t q (8a. btt aach is t tic that f quati (5 iicats that ( Da > always, s that th is iflcti it as th at f tmatu is ks isig util all actat is lt. h at x, fm q (5 it fllws that max a thf max a. W ca itgat th ifftial quati (5 by saatig th vaiabls t btai th citical valu f Da a, hc, f Da Da ( Da if γ ( + γ (9 laly f giv valus f aamts γ, β, βγ, a acti, w ca valuat if fm q (8a a th calculat th valu f Da by umically valuatig th itgal i q (9. Usig th th fiitis f Da a w gt th citi f saf ati which ca b xss as: Da < Da k R R ρ ( Δ H E Da ( gt a cvit, asy t mmb valu f Da, th fllwig aximatis a ft ma. Fist, th hius c f th at cstat tmatu is lac by a xtial c, i ffct γ ( + γ ( Substitutig this aximati i q (5 yils via q (7 t a w aximat valu f th tmatu at iflcti it ( if ( a Substitutig q ( a q ( it q (9 yils ( Da a u u u (3 4

he 47 Lctu Fall 5 h fial aximati (which is csvativ i atu as it assums th wst ssibl cas f zth acti igs th slww f th tmatu is u t th csumti f th actat, which is th sam as takig i q (3. his yils u u ( Da, u ( [ ] ( f lag ugh a (4 F highly xthmic actis a claly ( Da. a, Substitutig this it q ( givs th csvativ citi f saf ati. It is cstuctiv t t that this sam quati (a with tim t lacig k R R ρ ( Δ H E t < (a is us t tmi th s call tim f tu tim t xlsi i batch systms. his tim t iflcti it t may b vy lg f lw but bcms quit sht if th systm f high activati gy is xs t high. Hc, chmicals that may b saf t st at 5 may b xlsi if xs t 4 5! SFE OPERION OF DIBI SR h mass balac f a ivsibl -th acti is: x ( R (5 h aiabatic quati lats cvsi a tmatu x (6 ( Δ H ρ U substituti f imsilss tmatu w gt fm q (5 lt Da γ ( γ + (7 G ( ( γ + γ (8a 5

he 47 Lctu Fall 5 L (8b Da ( W kw fm bf that G is a sigmial cuv i a sts hat gat by acti. L is th hat mval at (i.., hat mv by ssibl hat f th flui that flws thugh th SR. W kw that u t th itsctis a ssibl btw G a L lis. avi th itscti laig t xcssivly high tmatus w must assu that itsctis at lw tmatus a availabl. h last missibl atig citi is th wh li L is als tagt t cuv G as schmatically shw i Figu. G L ( ( 3 3 FIGURE : Schmatic f th G, L vs. laly as Da icass th sl f th L li cass s that ( Da ( Da < ( Da 3 < (9 Whil atig aiabatic tmatus at a a acctabl, 3 sts t lag a tmatu jum. Hc, w must assu that th L li always itscts th G li at its lw tmatu bach. h citical it is ach wh L is als tagt t th G li. F saf aiabatic ati w thf qui 6

he 47 Lctu Fall 5 L G (3 L G (3 lyig th abv t qs (8a a (8b, a usig th quality sig i q (3, w gt th quati f th maximum missibl tmatu max m. h citical valu f th sac tim ca b btai fm th citical valu f Da, which i tu sults fm substitutig th xssi f it q (3. gt a siml, asy t mmb xssi, usually w agai lac yils γ ( + γ with. his ( + + 4 (3 h gativ sig i ft f th squa t s t b tak as w a itst i th lw f th tw tmatus at which th L li cul b tagt t th cuv G. h quati (3 yils: ( Da a (33 csvativ stimat, with, yils a Da (34 F saf ati th k ( Δ H E R R ρ (35 7