Chapter 13 Homework Answers

Similar documents
AP Chemistry--Chapter 12: Chemical Kinetics

Chapter 14 Homework Answers

CHEMICAL KINETICS: 1. Rate Order Rate law Rate constant Half-life Temperature Dependence

2) Of the following questions, which ones are thermodynamic, rather than kinetic concepts?

Chapter 14 Chemical Kinetics

Chapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws

Northern Arizona University Exam #1. Section 2, Spring 2006 February 17, 2006

Chapter 14 Chemical Kinetics

04. Kinetics of a second order reaction

Chapter 12. Chemical Kinetics

2. For a one-point fixed time method, a pseudo-first order reaction obeys the equation 0.309

CHAPTER 13 CHEMICAL KINETICS

CHEMICAL KINETICS Rate Order Rate law Rate constant Half-life Molecularity Elementary. Complex Temperature dependence, Steady-state Approximation

המחלקה : ביולוגיה מולקולרית הפקולטה למדעי הטבע

04. Kinetics of a second order reaction

A First Course on Kinetics and Reaction Engineering. Class 19 on Unit 18

CHAPTER 16 KINETICS: RATES AND MECHANISMS OF CHEMICAL REACTIONS

Chapter 7: Solving Trig Equations

EXERCISES FOR SECTION 1.5

Math 333 Problem Set #2 Solution 14 February 2003

APPM 2360 Homework Solutions, Due June 10

Some Basic Information about M-S-D Systems

ENV 6015 Solution to Mixing Problem Set

CHAPTER 12 DIRECT CURRENT CIRCUITS

Faculty of Natural Sciences and Technology RAPPORT. Felleslab, TKP 4105 og TKP 4110

Vehicle Arrival Models : Headway

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n

KINEMATICS IN ONE DIMENSION

ME 391 Mechanical Engineering Analysis

Reaction Order Molecularity. Rate laws, Reaction Orders. Determining Reaction Order. Determining Reaction Order. Determining Reaction Order

Solutionbank Edexcel AS and A Level Modular Mathematics

Suggested Problem Solutions Associated with Homework #5

Math 10B: Mock Mid II. April 13, 2016

Solutions to Assignment 1

Position, Velocity, and Acceleration

Advanced Organic Chemistry

LabQuest 24. Capacitors

Predator - Prey Model Trajectories and the nonlinear conservation law

Reading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4.

Phys1112: DC and RC circuits

Unsteady Mass- Transfer Models

5.1 - Logarithms and Their Properties

EE650R: Reliability Physics of Nanoelectronic Devices Lecture 9:

1. VELOCITY AND ACCELERATION

Navneet Saini, Mayank Goyal, Vishal Bansal (2013); Term Project AML310; Indian Institute of Technology Delhi

MA 214 Calculus IV (Spring 2016) Section 2. Homework Assignment 1 Solutions

System of Linear Differential Equations

Math 4600: Homework 11 Solutions

Homework 2 Solutions

KEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow

MA Study Guide #1

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x

3.6 Derivatives as Rates of Change

Brock University Physics 1P21/1P91 Fall 2013 Dr. D Agostino. Solutions for Tutorial 3: Chapter 2, Motion in One Dimension

Introduction to choice over time

Solution Kinetics of an Organic Reaction Amanda Nienow, adapted from Halpern 1

Motion along a Straight Line

Laplace transfom: t-translation rule , Haynes Miller and Jeremy Orloff

Econ107 Applied Econometrics Topic 7: Multicollinearity (Studenmund, Chapter 8)

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010

Elementary Differential Equations and Boundary Value Problems

6. Solve by applying the quadratic formula.

Lab 10: RC, RL, and RLC Circuits

Sterilization D Values

Cosumnes River College Principles of Macroeconomics Problem Set 1 Due January 30, 2017

- If one knows that a magnetic field has a symmetry, one may calculate the magnitude of B by use of Ampere s law: The integral of scalar product

u(x) = e x 2 y + 2 ) Integrate and solve for x (1 + x)y + y = cos x Answer: Divide both sides by 1 + x and solve for y. y = x y + cos x

Challenge Problems. DIS 203 and 210. March 6, (e 2) k. k(k + 2). k=1. f(x) = k(k + 2) = 1 x k

Exam 1 Solutions. 1 Question 1. February 10, Part (A) 1.2 Part (B) To find equilibrium solutions, set P (t) = C = dp

Chapter 2. First Order Scalar Equations

4.5 Constant Acceleration

EEEB113 CIRCUIT ANALYSIS I

Chapter 10 INDUCTANCE Recommended Problems:

The equation to any straight line can be expressed in the form:

Y 0.4Y 0.45Y Y to a proper ARMA specification.

MATH 31B: MIDTERM 2 REVIEW. x 2 e x2 2x dx = 1. ue u du 2. x 2 e x2 e x2] + C 2. dx = x ln(x) 2 2. ln x dx = x ln x x + C. 2, or dx = 2u du.

ln 2 1 ln y x c y C x

Physics 20 Lesson 5 Graphical Analysis Acceleration

WELCOME TO 1103 PERIOD 3. Homework Exercise #2 is due at the beginning of class. Please put it on the stool in the front of the classroom.

dy dx = xey (a) y(0) = 2 (b) y(1) = 2.5 SOLUTION: See next page

( ) ( ) ( ) + W aa. ( t) n t ( ) ( )

Math 334 Test 1 KEY Spring 2010 Section: 001. Instructor: Scott Glasgow Dates: May 10 and 11.

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities:

Assignment 6. Tyler Shendruk December 6, 2010

1 1 + x 2 dx. tan 1 (2) = ] ] x 3. Solution: Recall that the given integral is improper because. x 3. 1 x 3. dx = lim dx.

Nature Neuroscience: doi: /nn Supplementary Figure 1. Spike-count autocorrelations in time.

ENGI 9420 Engineering Analysis Assignment 2 Solutions

2.1: What is physics? Ch02: Motion along a straight line. 2.2: Motion. 2.3: Position, Displacement, Distance

Direct Current Circuits. February 19, 2014 Physics for Scientists & Engineers 2, Chapter 26 1

PET467E-Analysis of Well Pressure Tests/2008 Spring Semester/İTÜ Midterm Examination (Duration 3:00 hours) Solutions

Nuclear Decay kinetics : Transient and Secular Equilibrium. What can we say about the plot to the right?

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3

Matlab and Python programming: how to get started

NEWTON S SECOND LAW OF MOTION

5.2. The Natural Logarithm. Solution

Second order reactions. Second order, class I reactions 2A P A + B P. class I. class II. Nov 17, 2010!

Displacement ( x) x x x

Integration Over Manifolds with Variable Coordinate Density

Summary:Linear Motion

Transcription:

Chaper 3 Homework Answers 3.. The answer is c, doubling he [C] o while keeping he [A] o and [B] o consan. 3.2. a. Since he graph is no linear, here is no way o deermine he reacion order by inspecion. A secondorder reacion should exhibi linear behavior if a plo is made of /[A] vs ime. b. The daa seem o beer suppor a firsorder reacion. As he ime changes by 2 seconds, he concenraion of A decreases by 0 2. This is he behavior expeced for an exponenial rae law like a firsorder reacion rae law, [A] = [A] 0 e k. c. The rae consan is ln 2 /2 = 0.693 0.35 s =.980 =.98 /s d. A possible mechanism wih inermediaes X and Y is A X + Y (slow sep) X + Y B + C (fas sep) e. The behavior of he rae consan k as a funcion of emperaure is described by he Arrhenius equaion. k E ln 2 a = k R T T2 As he emperaure increases he rae consan also increases. More molecules collide wih sufficien energy o overcome he poenial energy barrier so he rae of reacion increases. 3.3. a. E mus be a produc since is concenraion increases wih ime. If E were a reacan, you would expec he concenraion o decrease over ime. b. The average rae is faser beween poins A and B because he slope of he curve is seeper in his region. Remember, he seeper he curve, he greaer he rae of change. 3.4. For he reacion 3I + H 3 AsO 4 + 2H + I 3 + H 3 AsO 3 + H 2 O, he rae of decomposiion of I and he rae of formaion of I 3 are, respecively, Rae = [I ]/ Rae = [I 3 ]/ To relae he wo raes, divide each rae by he coefficien of he corresponding subsance in he chemical equaion and equae hem. /3 [I ] = [I 3 ] 3.5. If he rae law is Rae = k[no] 2 [Cl 2 ], he order wih respec o NO is 2 (second order), and he order wih respec o Cl 2 is (firsorder). The overall order is 2 + = 3, hirdorder.

3.6. The reacion rae doubles when he concenraion of ehylene oxide is doubled, so he reacion is firs order in ehylene oxide. The rae equaion should have he form Rae = k[c 2 H 4 O] Subsiuing values for he rae and concenraion yields a value for k: rae [E. Ox.] = 7 5.57 x 0 M/s 3 2.72 x 0 M = 2.047 x 0 4 = 2.05 x 0 4 /s 3.7. By comparing Experimens 2 and 3, you see ha doubling [I ] doubles he rae, so he reacion is firs order in I. From Experimens and 3, you see ha doubling [ClO ] also doubles he rae, so he reacion is firs order in ClO. From Experimens 3 and 4, you see ha doubling [OH ] halves he rae; ha is, 2 m = /2. Hence m =, and he rae is inversely proporional o he firs power of OH. The rae law is Rae = k[i ][ClO ]/[OH ] Subsiuing values for he rae and concenraions yields a value for k: rae [OH ] [ClO ][I ] = 2 6. x 0 M/s [0.00 M ] [0.00 M] [0.00 M] = 6.0 = 6. /s 3.8. Firs, find he rae consan, k, by subsiuing experimenal values ino he firsorder rae equaion. Le [Cyb.] o = 0.0050 M, [Cyb.] = 0.009 M, and = 455 s. [0.009 M] k(455 s) = ln [0.0050 M] = 0.235 Solving gives 5.088 x 0 4 /s. Now le [Cyb.] = he concenraion afer 750 s and [Cyb.] o = 0.0050 M, and calculae [Cyb.]. [Cyb.] ln = (5.088 x 0 4 /s)(750 s) = 0.386 [0.0050 M] Taking he anilog of boh sides yields [Cyb.] = 0.68275 [0.0050 M] Solving for [Cyb.] gives [Cyb.] = 0.68275 x [0.0050 M] =.024 x 0 3 =.02 x 0 3 M 3.63. The rae consan for a secondorder reacion is relaed o he halflife by [A] /2 o Using a halflife of 425 s and an iniial A concenraion of 5.99 x 0 3 mol/l, he rae consan is 3 (425 s)(5.99 x 0 mol/l) = 0.3928 = 0.393 L/(mol s)

3.64. The rae law for a zeroorder reacion is [A] = k + [A] o. Using a ime of 4.3 x 0 2 s o go from an iniial concenraion of 0.50 M o 0.25 M, he rae consan is 0.25 M = k x 4.3 x 0 2 s + 0.50 M 0.50 M 0.25 M 2 4.3 x 0 s = 5.8 x 0 4 = 5.8 x 0 4 M/s 3.65. For he firsorder plo, follow Figure 3.9, and plo ln [MA], he mehyl aceae concenraion, versus ime in minues. This plo does no yield a sraigh line, so he reacion is no firs order. For he secondorder plo, follow Figure 3.0, and plo /[MA] versus ime in minues. The daa used for ploing are, min [MA], M /[MA] 0.00 0.0000 00.0 3.00 0.00740 35. 4.00 0.00683 46.4 5.00 0.00634 57.7 0.00 0.00463 25.9 20.00 0.00304 328.9 30.00 0.00224 446.4 The plo requires a graph wih oo many lines o be reproduced here, bu i yields a sraigh line, demonsraing ha he reacion is second order in [MA]. The slope of he line may be calculaed from he difference beween he las poin and he firs poin: Slope = [446.4 00.0]/ M.54 = [30.00 0.00]min M min = 0.92 s M In his case, he slope equals he rae consan, so.5/(m m), or 0.92/(M s). 3.66. For ploing ln k versus /T, he daa below are used: k ln k /T (K) 2.69 x 0 3 5.98.402 x 0 3 6.2 x 0 3 5.08.364 x 0 3.40 x 0 2 4.268.328 x 0 3 3.93 x 0 2 3.236.294 x 0 3 The plo yields an approximaely sraigh line. The slope of he line may be calculaed from he difference beween he las poin and he firs poin: (3.236) (5.98) Slope = 3 3 [.294 x 0.402 x 0 ]/K = 2.483 x 04 K Because he slope = E a /R, you can solve for E a using R = 8.3 J/K mol: Ea = 2.483 x 0 4 K 8.3 J/ (K mol) E a = 2.483 x 0 4 K x 8.3 J/K mol = 2.063 x 0 5 J/mol (2. x 0 2 kj/mol)

3.67. All raes of reacion are calculaed by dividing he decrease in concenraion by he difference in imes; only he seup for he firs rae afer.0 min is given below: (0.076 0.03) M Rae (.0 min) = (.0 0) min x min 60 s = 4.50 x 0 5 = 4.5 x 0 5 M/s A summary of he imes and raes is given in he able. Time, min Rae 3.68..0 4.50 x 0 5 = 4.5 x 0 5 M/s 2.0 4.33 x 0 5 = 4.3 x 0 5 M/s 3.0 4.00 x 0 5 = 4.0 x 0 5 M/s a. A plo of /[A] versus ime is a sraigh line for a secondorder reacion. b. The secondorder inegraed rae law is [A] = k + [A] o Afer 57 s, he concenraion of A dropped 40% of is iniial value, so [A] = 0.60[A] o, or (0.60)(0.50 M) = 0.30 M. Using hese values gives 0.30 mol/l = k x (57 s) + 0.50 mol/l k x (57 s) = 0.30 mol/l 0.50 mol/l =.333 L/mol.333 L/mol 57 s = 0.0233 = 0.023 L/(mol s) 3.69. Facors ha affec he raes of reacions: i) Concenraions of he reacans ii) Temperaure iii) Caalyss A higher concenraions, more molecules can undergo effecive collisions and give more produc per uni of ime. The emperaure affecs he number of molecules ha have enough energy o reac. The higher he emperaure, he larger he fracion of molecules ha have enough energy o reac. Caalyss provide anoher pahway for reacion ha has a lower acivaion energy, so more molecules have he minimum energy o reac. The value of he rae consan for a paricular reacion depends on he emperaure and he acivaion energy. The concenraion of caalys and of he solven, if he reacion occurs in soluion, can affec E a. 3.29. a. The overall reacion is 2H 2 O 2 2H 2 O + O 2 b. The caalys is I, and he inermediae is IO. c. No, he rae law can no be specified unil he raedeermining sep is esablished.

3.30. The balanced equaion is 2H 2 O 2 2H 2 O + O 2. Noe ha he moles of O 2 formed will be equal o onehalf ha of he moles of H 2 O 2 decomposed. Now, use he inegraed form of he firsorder rae law o calculae he fracion of he.00 mol H 2 O 2 decomposing in 20.0 min, or 200 s. [H2O 2] ln = k = (7.40 x 0 4 /s)(200 s) = 0.8880 [H O ] 2 2 o [H2O 2] [H O ] 2 2 o = e 0.8880 = 0.447 Fracion of H 2 O 2 decomposed =.00 0.447 = 0.58852 Since here is.00 mol of H 2 O 2 presen a he sar, he moles of H 2 O 2 decomposed are 0.58852 mol. Thus, Moles of O 2 formed = ( O 2 /2 H 2 O 2 ) x 0.58852 mol H 2 O 2 = 0.29426 mol O 2 Now, use he ideal gas law o calculae he volume of his number of moles of O 2 gas a 25 C and 740 mmhg. V = nrt P (0.29426 mol)(0.08206 L am/(k mol))(298 K) = (740/ 760) am = 7.39 = 7.4 L