LECTURE 4 Variation of enthalpy with temperature

Similar documents
Thermochemistry: Heat and Chemical Change

Homework Problem Set 6 Solutions

ENTHALPY CHANGE CHAPTER 4

Lecture 7 Enthalpy. NC State University


Chapter 5 Practice Multiple Choice & Free

Enthalpy. Enthalpy. Enthalpy. Enthalpy. E = q + w. Internal Energy at Constant Volume SYSTEM. heat transfer in (endothermic), +q

Thermochemistry: Energy Flow and Chemical Reactions

Enthalpies of Reaction

Chapter 8. Thermochemistry 강의개요. 8.1 Principles of Heat Flow. 2) Magnitude of Heat Flow. 1) State Properties. Basic concepts : study of heat flow

8.6 The Thermodynamic Standard State

CHAPTER 3 THE FIRST LAW OF THERMODYNAM- ICS

Name Date Class THE FLOW OF ENERGY HEAT AND WORK

I PUC CHEMISTRY CHAPTER - 06 Thermodynamics

Chapter 8 Thermochemistry: Chemical Energy

17.2 Thermochemical Equations

Chapter 6 The States of Matter. Examples of Physical Properties of Three States of Matter

Chapter 5 Principles of Chemical Reactivity: Energy and Chemical Reactions

Exothermic process is any process that gives off heat transfers thermal energy from the system to the surroundings. H 2 O (l) + energy

Chapter 8. Thermochemistry

CH10007/87. Thermodynamics. Dr Toby Jenkins

Measuring and Expressing Enthalpy Changes. Copyright Pearson Prentice Hall. Measuring and Expressing Enthalpy Changes. Calorimetry

Chemical Thermodynamics

Ch. 6 Enthalpy Changes

Quantity Relationships in Chemical Reactions

Chapter 11. Intermolecular Forces, Liquids, and Solids

FACULTY OF SCIENCE MID-TERM EXAMINATION CHEMISTRY 120 GENERAL CHEMISTRY MIDTERM 1. Examiners: Prof. B. Siwick Prof. I. Butler Dr. A.

AAE THERMOCHEMISTRY BASICS

Thermochemistry. Energy. 1st Law of Thermodynamics. Enthalpy / Calorimetry. Enthalpy of Formation

Name Chemistry / / SOL Questions Chapter 9 For each of the following, fill in the correct answer on the BLUE side of the scantron.

Thermochemistry Chapter 4

Chapter 12 Intermolecular Forces of Attraction

6.Thermodynamics. Some Important Points and Terms of the Chapter

Calorimetry &Thermochemistry

Chapter 8 Thermochemistry

CHM 111 Dr. Kevin Moore

Energy Heat Work Heat Capacity Enthalpy

General Chemistry 1 CHM201 Unit 3 Practice Test

Class XI Chapter 6 Thermodynamics Chemistry

Energetics. These processes involve energy exchanges between the reacting system and its surroundings.

Homework 01. Phase Changes and Solutions

_ + Units of Energy. Energy in Thermochemistry. Thermochemistry. Energy flow between system and surroundings. 100º C heat 50º C

Energy is the capacity to do work

Thermochemistry: the study of energy (in the from of heat) changes that accompany physical & chemical changes

Entropy Changes & Processes

Thermochemistry Chapter 8

Unit 7 Thermochemistry Chemistry 020, R. R. Martin

Energy, Heat and Chemical Change

Module 5: Combustion Technology. Lecture 32: Fundamentals of thermochemistry


Section 9: Thermodynamics and Energy

THERMODYNAMICS READ THE INSTRUCTIONS CAREFULLY

Mr Chiasson Advanced Chemistry 12 / Chemistry 12 1 Unit B: Thermochemical Changes

Contents and Concepts

TERMS AND DEFINITIONS IN THERMOCHEMISTRY

Page 1 of 11. Website: Mobile:

Chemical Thermodynamics

Chapter Objectives. Chapter 9 Energy and Chemistry. Chapter Objectives. Energy Use and the World Economy. Energy Use and the World Economy

Energy: Heat, Nutrients, and Enthalpy Page 13

The Nature of Energy Energy is the ability to do work or produce Heat, q or Q, is ; flows due to temperature differences (always to )

Date: SCH 4U Name: ENTHALPY CHANGES

Chemistry Chapter 16. Reaction Energy

Topic 5: Energetics. Heat & Calorimetry. Thursday, March 22, 2012

Chapter 11. Thermochemistry. 1. Let s begin by previewing the chapter (Page 292). 2. We will partner read Pages

Chemistry B11 Chapter 6 Gases, Liquids, and Solids

Chapter 14. Liquids and Solids

Slide 1 / Objects can possess energy as: (a) endothermic energy (b) potential energy (c) kinetic energy. a only b only c only a and c b and c

CHAPTER 16 REVIEW. Reaction Energy. SHORT ANSWER Answer the following questions in the space provided.

Thermochemistry. Section The flow of energy

Entropy, Free Energy, and Equilibrium

Name: General Chemistry Chapter 11 Thermochemistry- Heat and Chemical Change

Energetics. Topic

I. The Nature of Energy A. Energy

June Which is a closed system? (A) burning candle (B) halogen lightbulb (C) hot water in a sink (D) ripening banana

Free-energy change ( G) and entropy change ( S)

Thermodynamics. Heat Capacity Calorimetry Enthalpy Thermodynamic cycles Adiabatic processes. NC State University

Chapter 8 Thermochemistry: Chemical Energy. Chemical Thermodynamics

Chemistry Slide 1 of 33

(g) + 3H 2. (g) 2NH 3. (g) (a) Explain what is meant by a dynamic equilibrium. (2)

Chapter 17: Energy and Kinetics

AP CHEMISTRY NOTES 8-1 CHEMICAL EQUILIBRIUM: AN INTRODUCTION

Thermochemistry. Chapter 6. Concept Check 6.1. Concept Check 6.2. Solution

Thermodynamics- Chapter 19 Schedule and Notes

The table below includes some values of standard enthalpies of formation ( H ).

(E) half as fast as methane.

Entropy Changes & Processes

CHEMISTRY LEVEL 4C (CHM415115)

Name Class Date. As you read Lesson 17.1, use the cause and effect chart below. Complete the chart with the terms system and surroundings.

0. Graphite is thermodynamically less stable that diamond under standard conditions. 1. True 2. False

Enthalpy Chapter 5.3-4,7

1.4 Enthalpy. What is chemical energy?

Thermochemistry-Part 1

Lecture 20. Phase Transitions. Phase diagrams. Latent heats. Phase-transition fun. Reading for this Lecture: Elements Ch 13.

U N I T T E S T P R A C T I C E

Chapter 11. Liquids and Intermolecular Forces

Chapter 17: Spontaneity, Entropy, and Free Energy

Exam 4, Enthalpy and Gases

exothermic reaction and that ΔH c will therefore be a negative value. Heat change, q = mcδt q = m(h 2

Thermodynamics - Energy Relationships in Chemical Reactions:

Chemistry Lab Fairfax High School Invitational January 7, Team Number: High School: Team Members Names:

Transcription:

LECTURE 4 Variation of enthalpy with temperature So far, we can only work at 25 C. Like c v we define a constant pressure heat capacity, c p, as the amount of heat energy needed to raise the temperature of 1 mole of substance by 1 K at constant pressure. c p dq p dh = = dt dt p p or dh = c p dt Thus, H must increase by (c p dt) if heated by dt. T dh = c dt T 2 1 p the Kirchoff Equation First approximation: treat c p as independent of T for small temp. ranges or use the average value over the range of T H H = c ( T T ) T T p 2 1 2 1 Particularly useful: recall that standard enthalpies of formation are defined at 25 C. Hence, we can write H f, T = H f, 298 + c p ( T - 298.15 )

Enthalpies of Reaction A model reaction: R P The enthalpy of R at 25 C is H f, 298 (R). The enthalpy at some other temperature T is [ H f, 298 (R) + c p (R) (T - 298.15)]. H T (reaction) = [ H f, T (P) ] [ H f, T (R)] = [ H f, 298 (P) + c p (P) (T 298.15)] [ H f, 298 (R) + c p (R) (T 298.15)] = [ H f, 298 (P) - H f, 298 (R)} + {[ c p (P) - c p (R)] (T 298.15)} or H T (reaction) = H 298 (reaction) + c p (T - 298.15) where c p = ν i p ν i p c (products) - c (reactants)

The complete combustion of ethane releases 1558.8 kj mol -1 at 25 C. Calculate H (combustion) at 100 C. c p / J K -1 mol -1 : C 2 H 6(g) 52.6; O 2(g) 29.4; CO 2(g) 37.1; H 2 O (l) 75.3. C 2 H 6(g) + 3½ O 2(g) 2 CO 2(g) + 3 H 2 O (l) H 298 = - 1558.8 kj mol -1 c p = [2 c p (CO 2 ) + 3 c p (H 2 O)] - [c p (C 2 H 6 ) + 3½ c p (O 2 )] = [2 (37.1) + 3 (75.3)] - [ 52.6 + 3½ (29.4)] = 144.6 J K -1 mol -1 H 373 = H 298 + c p T = - 1558.8 x 10 3 (J mol -1 ) + (144.6 J K -1 mol -1 )(75 K) = - 1547.9 kj mol -1

Other types of enthalpy change Enthalpy of combustion - often referred to as the Heat of combustion the enthalpy change when 1 mol of a compound reacts completely with excess oxygen gas. e.g. the combustion of 1 mol of methane gas at 25 C evolves 890.3 kj. CH 4(g) + 2O 2(g) CO 2(g) + 2H 2 O (l) H 298 (comb.) = -890.3 kj mol -1 H 298 (combust) are easy to measure and often used to determine H f,298 values. e.g. combustion of methane CH 4(g) + 2 O 2(g) CO 2(g) + 2 H 2 O (l) H (comb) = [2 H f (H 2 O) + H f (CO 2 )]-[ H f (CH 4 ) + 2 H f (O 2 )] -890.3 = [2 (-285.8) + (-393.5] - [ H f (CH 4 ) + 2 (0)] -890.3 = -965.1 - H f (CH 4 ) H f (CH 4 ) = 74.8 kj mol -1

The bomb calorimeter - already seen for U(combustion) at constant volume H(combustion) = U(combustion) + (pv) (combustion) If the gases behave ideally (pv) = (pv) prod - (pv) react = RT {(n gas ) prod - (n gas ) react } (pv) = n gas R T H(comb.) = U(comb.) + n gas R T where n gas is the number of moles of gas involved in the reaction. Why do we only consider gases? Volume of 1 mol of ideal gas: 25 C, 1 atm = 24470 cm 3. At 25 C: water occupies ~18 cm 3 mol -1 ; hexane 132 cm 3 mol -1, benzene 89 cm 3 mol -1 and naphthalene 120 cm 3 mol -1. Volumes of solids and liquids are negligible.

An example Following the earlier calculation, calculate the enthalpy of combustion of naphthalene at 25 C. From earlier, U(comb.) for naphthalene at 25 C = - 5142 kj mol -1 C 10 H 8 (s) + 12 O 2 (g) 10 CO 2 (g) + 4 H 2 O (l) To convert H to U using Eqn. 2.a, we need n gas. n gas = n gas (products) - n gas (reactants) = 10-12 = -2 mol H(comb.) = - 5142000 J mol -1 + (-2 mol) (8.314 J K -1 mol -1 ) (298.2 K) H(combustion) = - 5147000 J mol -1 = - 5147 kj mol -1 Exercise: Take the values from Example 2.8 and calculate the error in neglecting the volumes of naphthalene and water.

Note that the difference between the internal energy and enthalpy is relatively small in this case. Enthalpies of phase change Consider S, L, G for now. solid to liquid: melting or fusion. Liquid molecules have greater motion than solid - energy has to be added to the solid - fusion is an endothermic process. The enthalpy of fusion, H fus is the energy required at 1 bar pressure to melt 1 mole of a pure component at its melting point, T m. An earlier name, still in common usage is that H fus is the latent heat of fusion. It essentially represents the energy needed to overcome the intermolecular forces in the solid, Also, H(freezing) = - H(fusion)

liquid vapour - vaporization. H vap is the energy required at 1 bar pressure to vaporize 1 mole of a pure liquid at its boiling point, T b. Vaporisation is also endothermic. H vap is considerable larger than H fus since the molecules are completely separated in vaporization whereas a considerable degree of intermolecular interaction remains in liquids. Solid vapour - sublimation. Some compounds do not display a liquid phase an example is solid carbon dioxide which, at atmospheric pressure, sublimates at -78 C. H(sublimation) = H(fusion) + H(vaporization)

Examples Calculate the energy required to turn 100 g of ice at 0 C into steam at 100 C. The process required can be conveniently split into three parts. 1. 100 g ice 100 g water at 0 C H 1 = H fus for 100 g 2. 100 g water, 0 C 100 g water, 100 C H 2 = c p T for 100 g 3. 100g water, 100 C 100g steam, 100 C H 3 = H vap for 100 g 100 g of water = 100 / 18 mol = 5.56 mol H total = H 1 + H 2 + H 3 = 5.56 mol [ + 6.01 x 10 3 + 75.1 (373-273) + 40.7 x 10 3 ] = 301.46 kj (100g) -1 Note that the factor of 10 3 occurs in H 1 and H 3 since they are measured in kj mol -1 while c p is in J K -1 mol -1.

A gas mixture consisting of 25% nitrogen and 75% hydrogen (by volume) was passed over a catalyst at a rate of 112 dm 3 min -1 (Gas volumes corrected to 0 C and 1 atm pressure). The reaction took place at 450 C and 1 bar pressure and complete conversion to ammonia was achieved. Given the following data, calculate the rate of heat evolution or absorption. H f, 298 (NH 3 ) - 46.0 kj mol -1 Mean c p / J K -1 mol -1 : N 2 29.7; H 2 29.3; NH 3 39.7. The enthalpy change at 25 C can be calculated N 2(g) + 3 H 2(g) 2 NH 3(g) H 298 = [ 2 x H f, 298 (NH 3 )] - [ H f, 298 (N 2 ) + 3 H f, 298 (H 2 )] = [ - 92.0 ] - [ 0 ] kj mol -1 H 298 = - 92.0 kj mol -1 Correcting the enthalpy change to 450 C makes use of the Kirchoff Eqn. H T (reaction) = H 298 (reaction) + c p (T - 298.15) c p = [2 x c p (NH 3 )] - [ c p (N 2 ) + 3 x c p (H 2 )} = [2 x 39.7] - [ 29.7 + (3 x 29.3)] = - 38.2 J K -1 mol -1 H 723 = - 92000 Jmol -1 + (- 38.2 J K -1 mol -1 ) (723.15-298.15)K = - 92000 Jmol -1 + ( - 16235 Jmol -1 ) H 723 = - 108.24 kj mol -1 Hence, at 450 C, 108.24 kj is evolved for each mole of the equation as written. From the stoichiometry, this means that 108.24 kj is evolved per mole of nitrogen which reacts. Since, for a gas, the volume is proportional to the number of moles, the 1:3 mixture is in the stoichiometric amount. We know that at 0 C and 1 atm pressure, 1 mole of an ideal gas

occupies 22.4 dm 3. Thus, the total amount of gas passing over the catalyst amounted to 5 moles per minute, of which 1.25 moles were N 2. Rate of heat evolution = (moles of N 2 min -1 ) (heat evolved per mole N 2 ) = ( 1.25 mol min -1 ) (- 108.24 kj (mol N 2-1 ) = - 135.3 kj min -1 The negative sign indicates an exothermic reaction so that heat is evolved.

Using the data from a text, estimate the standard enthalpies of formation for (a) gaseous cyclohexane, C 6 H 12 and (b) gaseous benzene, C 6 H 6. Compare the true values in a data table. (a) The formation of cyclohexane can be written 6 C (graph) + 6 H 2(g) C 6 H 12(g) H 1 = H f (C 6 H 12(g) ) To form cyclohexane, we need to make 6 C C bonds and 12 C H bonds. From the definition of bond energies, this refers to the reaction 6 C (g) + 12 H (g) C 6 H 12(g) H 2 = 6 (-344) + 12 (-415) = -7044 kj mol -1 the values being negative since this is the reverse of bond dissociation. Prior to this step, we need 6 C (graph) + 6 H 2(g) 6 C (g) + 12 H (g) H 3 = 6 H (graph.) + 6 H (H H) H 3 = 6 (716.7) + 6 (436) = 6916.2 kj mol -1. It is clear that H 1 = H 2 + H 3 = -7030 + 6916.2 = -127.8 kj mol -1 The actual value is -123.2 kj mol -1. The agreement is therefore very good considering that average bond energies have been used throughout. (b) This calculation is performed in an analogous manner to part (a) except that benzene contains 6 C H, 3 C C and 3 C=C bonds. 6 C (graph) + 3 H 2(g) C 6 H 6(g) H 1 = H f (C 6 H 12(g) ) 6 C (g) + 6 H (g) C 6 H 6(g) H 2 = 3 (- 615) + 3 (-344) + 6 (-415) = -5367 kj mol -1

6 C (graph) + 3 H 2(g) 6 C (g) + 6 H (g) H 3 = 6 H (graph.) + 6 H (H H) H 3 = 6 (716.7) + 3 (436) = 5608.2 kj mol -1. It is clear that H 1 = H 2 + H 3 = -7030 + 6916.2 = 241.2 kj mol -1 The actual value is 83 kj mol -1. Clearly, there is poor agreement for benzene. This is due to the assumption of the alternating single and double bonds in benzene whereas the actual structure is a resonance stabilised hybrid of these. Note: This illustrates that care must be taken to consider the chemical properties of the molecules involved when using average bond enthalpy data. At best approximate results can be expected. The complete combustion of 2.0026 g of sucrose (C 12 H 22 O 11) in a bomb calorimeter with a heat capacity of 11140 JK -1 25 C resulted in a temperature increase of 2.966 C. Calculate H combustion for sucrose. at The energy released on combustion is given by (11140 JK -1 2.966 K) = 33.041 kj Since the bomb calorimeter is a constant volume device, this gives U combustion. The experiment used 5.85 x 10-3 moles. Hence, U combustion = - 33.041 / 5.85 x 10-3 = - 5647.5 kj mol -1 The chemical equation for the reaction is C 12 H 22 O 11(s) + 12 O 2(g) 12 CO 2(g) + 11 H 2 O (l) so the number of moles of gas is the same before and after the reaction. Hence, n gas = 0 and H combustion = U combustion H combustion = - 5647.5 kj mol -1