Fuel, Air, and Combustion Thermodynamics

Similar documents
Fuel and Air Flow in the Cylinder

Dr Ali Jawarneh Department of Mechanical Engineering Hashemite University

Reacting Gas Mixtures

ME 354 Tutorial, Week#13 Reacting Mixtures

Gestão de Sistemas Energéticos 2017/2018

Chapter 15. In the preceding chapters we limited our consideration to CHEMICAL REACTIONS. Objectives

Using first law of thermodynamics for a constant pressure system: Using first law of thermodynamics for a constant volume system:

Index to Tables in SI Units

FUNDAMENTALS of Thermodynamics

INTERNAL COMBUSTION ENGINE (SKMV 3413)

Combustion: Flame Theory and Heat Produced. Arthur Anconetani Oscar Castillo Everett Henderson

ME 201 Thermodynamics

Lecture 37. Heat of Reaction. 1 st Law Analysis of Combustion Systems

AAE COMBUSTION AND THERMOCHEMISTRY

1. (25 points) C 6 H O 2 6CO 2 + 7H 2 O C 6 H O 2 6CO + 7H 2 O

DISCIPLINA MIEEA 2018

MAE 11. Homework 8: Solutions 11/30/2018

Pure Substance. Properties of Pure Substances & Equations of State. Vapour-Liquid-Solid Phase Equilibrium

Thermodynamics I Chapter 2 Properties of Pure Substances

Thermochemistry X.S. Bai Thermochemistry

Chapter 6. Using Entropy

FUNDAMENTALS OF THERMODYNAMICS

COMBUSTION OF FUEL 12:57:42

Stoichiometry, Energy Balances, Heat Transfer, Chemical Equilibrium, and Adiabatic Flame Temperatures. Geof Silcox

R13. II B. Tech I Semester Regular Examinations, Jan THERMODYNAMICS (Com. to ME, AE, AME) PART- A

Combustion. Indian Institute of Science Bangalore

2SO 2(g) + O 2(g) Increasing the temperature. (Total 1 mark) Enthalpy data for the reacting species are given in the table below.

I.C. Engine Cycles. Thermodynamic Analysis

0 o C. H vap. H evap

Basic Thermodynamics Module 1

Chapter 3 PROPERTIES OF PURE SUBSTANCES. Thermodynamics: An Engineering Approach, 6 th Edition Yunus A. Cengel, Michael A. Boles McGraw-Hill, 2008

N L N G : C O M B U S T I O N

Thermochemistry Chapter 8

PROBLEM 6.3. Using the appropriate table, determine the indicated property. In each case, locate the state on sketches of the T-v and T-s diagrams.

Pure Substance. Properties of Pure Substances & Equations of State. Vapour-Liquid-Solid Phase Equilibrium

Thermodynamics Qualifying Exam Study Material

Dr Ali Jawarneh. Hashemite University

Introduction to Chemical Engineering Thermodynamics. Chapter 4. KFUPM Housam Binous CHE 303

R13 SET - 1 '' ''' '' ' '''' Code No RT21033

Modeling for Control of HCCI Engines

The Advanced Chemical Engineering Thermodynamics. The thermodynamics properties of fluids (II) Ji-Sheng Chang Q&A_-10-11/17/2005(10)

What s free about Gibbs free energy?

Chapter Eighteen. Thermodynamics

THERMODYNAMICS, FLUID AND PLANT PROCESSES. The tutorials are drawn from other subjects so the solutions are identified by the appropriate tutorial.

II/IV B.Tech (Regular) DEGREE EXAMINATION. (1X12 = 12 Marks) Answer ONE question from each unit.

CHAPTER 7 ENTROPY. Copyright Hany A. Al-Ansary and S. I. Abdel-Khalik (2014) 1

and mol of Cl 2 was heated in a vessel of fixed volume to a constant temperature, the following reaction reached equilibrium.

ME Thermodynamics I

KNOWN: Pressure, temperature, and velocity of steam entering a 1.6-cm-diameter pipe.

Chapter 20. Heat Engines, Entropy and the Second Law of Thermodynamics. Dr. Armen Kocharian

Use the data in the table to calculate the standard enthalpy of formation of liquid methylbenzene, C 7 H 8. Substance C(s) H 2 (g) C 7 H 8 (l)

Stoichiometry Rockets

Version 001 HW 15 Thermodynamics C&J sizemore (21301jtsizemore) 1

Conservation of mass: 44 kg on LHS and RHS one kmol of CO₂ produced by burning 1 kmol of C with one kmol of O₂

CHEMISTRY Topic #2: Thermochemistry and Electrochemistry What Makes Reactions Go? Fall 2018 Dr. Susan Findlay See Exercises in Topic 8

MODULE TITLE : MASS AND ENERGY BALANCE TOPIC TITLE : ENERGY BALANCE TUTOR MARKED ASSIGNMENT 3

Laws of Thermodynamics

+ m B1 = 1. u A1. u B1. - m B1 = V A. /v A = , u B1 + V B. = 5.5 kg => = V tot. Table B.1.

Lecture 40: Air standard cycle, internal combustion engines, Otto cycle

First Law of Thermodynamics

Dishwasher. Heater. Homework Solutions ME Thermodynamics I Spring HW-1 (25 points)

THE FIRST LAW APPLIED TO STEADY FLOW PROCESSES

Heat Engine Cycles. Chapter 2

MAE 320 THERODYNAMICS FINAL EXAM - Practice. Name: You are allowed three sheets of notes.

Teaching schedule *15 18

Chem 105/107 Exam #3 Fall 2012

Thermodynamics is the study of the relationship between heat and other forms of energy that are involved in a chemical reaction.

Name: I have observed the honor code and have neither given nor received aid on this exam.

UNIT I Basic concepts and Work & Heat Transfer

Ph.D. Qualifying Examination In Thermodynamics

Thermodynamic and Stochiometric Principles in Materials Balance

Name: Discussion Section:

1. (10) Calorically perfect ideal air at 300 K, 100 kpa, 1000 m/s, is brought to rest isentropically. Determine its final temperature.

Chemical Energetics. First Law of thermodynamics: Energy can be neither created nor destroyed but It can be converted from one form to another.

Energy, Enthalpy and Thermochemistry. Energy: The capacity to do work or to produce heat

CHAPTER 8 ENTROPY. Blank

Chapter 3 PROPERTIES OF PURE SUBSTANCES

ME Thermodynamics I = = = 98.3% 1

Theory. Humidity h of an air-vapor mixture is defined as the mass ratio of water vapor and dry air,

CHEM Exam 2 - October 11, INFORMATION PAGE (Use for reference and for scratch paper)

Problem 1 (Willans Approximation)

Chapter 3 PROPERTIES OF PURE SUBSTANCES

The need for something else: Entropy

Chapter One Reviews of Thermodynamics Update on 2013/9/13

Chapter 3 PROPERTIES OF PURE SUBSTANCES SUMMARY

A Project for Thermodynamics II. Entitled

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad

Find: a) Mass of the air, in kg, b) final temperature of the air, in K, and c) amount of entropy produced, in kj/k.

ENTHALPY BALANCES WITH CHEMICAL REACTION

Chapter 6 Problems: 9, 19, 24, 25, 26, 27, 31-33, 37, 39, 43, 45, 47, 48, 53, 55, 57, 59, 65, 67, 73, 78-82, 85, 89, 93

Pure Substances Phase Change, Property Tables and Diagrams

III. Evaluating Properties. III. Evaluating Properties

Speed Distribution at CONSTANT Temperature is given by the Maxwell Boltzmann Speed Distribution

ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER. 13 June 2007

5.4 Liquid Mixtures. G i. + n B. = n A. )+ n B. + RT ln x A. + RT ln x B. G = nrt ( x A. ln x A. Δ mix. + x B S = nr( x A

MathCAD Functions for Thermodynamic Analysis of Ideal Gases

Thermal Energy Final Exam Fall 2002

ME Thermodynamics I

AP Chemistry A. Allan Chapter Six Notes - Thermochemistry

Chemical Thermodynamics

Transcription:

Chapter 3 Fuel, Air, and Combustion Thermodynamics 3.1) What is the molecular weight, enthalpy (kj/kg), and entropy (kj/kg K) of a gas mixture at P = 1000 kpa and T = 500 K, if the mixture contains the following species and mole fractions? a) A table of the given and computed parameters is: i y i M i h o f h i h o f s o i ( y i s o i R u ln(y i ) ) [ kg /kmol] [ MJ /kmol] [ MJ /kmol] [ kg /kmol K] [ kj /kmol K] CO 2 1 0.10 44.01-393.52 33.40 269.30 28.84 H 2 O 2 0.15 18.01-241.83 26.00 232.74 37.28 N 2 3 0.70 28.01 0 21.46 228.17 161.79 CO 4 0.05 28.01-110.53 21.69 234.54 12.97 The mixture molecular mass is: M = y i M i = (0.10)(44.01) + (0.15)(18.01) + (0.70)(28.01) + (0.05)(28.01) M = 28.11 kg /kmol The specific mixture enthalpy is: h f = y i h i = (0.10)( 393.52 + 33.40) + (0.15)( 241.83 + 26.00) The mixture enthalpy is: + (0.70)(0 + 21.46) + (0.05)( 110.53 + 21.69) h f = 57.8 MJ /kmol = 5.78 10 4 kj/kmol h = h 5.78 104 = m 28.11 h = 2056 kj /kg The specific mixture entropy is: ( ) P s = R u ln + y i (s o i R u ln(y i )) P 0 ( ) 1000 s = ( 8.314) ln + 28.84 + 37.28 + 161.79 + 12.97 100 s = 221.74 kj /kmol K 1

2 CHAPTER 3. FUEL, AIR, AND COMBUSTION THERMODYNAMICS The mixture entropy is: s = s m = 103.23 28.11 s = 7.888 kj /kg K

3 3.2) What is the enthalpy h (kj/kg) and entropy s (kj/kg-k) of a mixture of 30% H 2 and 70% CO 2 by volume at a temperature of 3000 K? a) A table of the given and computed parameters is: i y i M i h o f h i h o f s o i ( y i s o i R u ln(y i ) ) [ kg /kmol] [ MJ /kmol] [ MJ /kmol] [ kg /kmol K] [ kj /kmol K] CO 2 1 0.70 44.01-393.52 152.85 334.17 235.99 H 2 2 0.30 2.016 0 88.72 202.90 63.87 The mixture molecular mass is: M = y i M i = (0.70)(44.01) + (0.30)(2.016) M = 31.41 kg /kmol The specific mixture enthalpy is: h f = y i h i = (0.70)( 393.52 + 152.85) + (0.30)(0 + 88.73) = 14.8 MJ /kmol = 1.418 10 5 kj/kmol The mixture enthalpy is: h = h 1.418 105 = m 31.41 h = 4516 kj /kg The specific mixture entropy is: ( ) P s = R u ln + y i (s o i R u ln(y i )) P 0 ( ) 2000 s = ( 8.314) ln + 235.99 + 63.87 100 s = 296.86 kj /kmol K The mixture entropy is: s = s m = 296.86 31.41 s = 9.451 kj /kg K

4 CHAPTER 3. FUEL, AIR, AND COMBUSTION THERMODYNAMICS 3.3) Using the Gordon and McBride equations, Equations (3.38) and (3.39), calculate the enthalpy h and entropy s o of CO 2 and compare with the gas table values used in Example 3.1. A Matlab program for calculating the enthalpy h and entropy s o of CO 2 is t=1000; % temp in K R=8.31451 % univ. gas const. a1=2.4007797; a2=8.73509757e-3; a3=-6.60707878e-6; a4=2.0021861e-9; a5=6.3274039e-16; a6=-4.8377527e4; a7=9.6951457; nondimh=a1+a2/2*t+a3/3*t^2+a4/4*t^3+a5/5*t^4+a6/t h=nondimh*t*r nondims=a1*log(t)+a2*t+a3/2*t^2+a4/3*t^3+a5/4*t^4+a7 s=nondims*r The calculated h = 3.6011 10 5 kj/kmol and the entropy s o = 269.21 kj/kmol-k. The gas table values are h = 3.6012 10 5 kj/kmol and the entropy s o = 269.30 kj/kmol-k. The enthalpy values agree to 4 figures, and the entropy values agree to 3 figures.

3.4) Using the program Fuel.m, at what temperature is the specific heat c p of methane CH 4 = 3.0 kj/kg-k? 5

6 CHAPTER 3. FUEL, AIR, AND COMBUSTION THERMODYNAMICS 3.5) Why does Equation 3.27 contain y i? a) From the Gibbs equations, we have ( ) s i (T, P ) = s o Pi i (T ) R i ln P 0 Where s o i (T ) is the standard entropy. y i = P i P = P i P0 P 0 P ( ) ( ) Pi P0 ln(y i ) = ln + ln P 0 P ( ) ( ) Pi P ln = ln(y i ) + ln P 0 Substituting back in: ( )) P s i (T, P ) = s o i (T ) R i (ln(y i ) + ln The mole fraction y i originates from the pressure ratio term. P 0 P 0

7 3.6) A system whose composition is given below is in equilibrium at P = 101 kpa and T = 298 K. What are the enthalpy (kj/kg), specific volume (m 3 /kg), and quality χ of the mixture? a) A table of the given and computed parameters is: i y i M i h f h i x i [ v i ] [ kg /kmol] [ kj /kmol] [ kj /kg] m 3 /kg H 2 O 1 0.141 18.01-241,826-13,424 0.0888 1.362 CO 2 2 0.125 44.01-393,522-8942 0.1924 0.557 N 2 3 0.734 28.01 0 0 0.7189 0.875 The mixture molecular mass is: M = y i M i = (0.141)(18.01) + (0.125)(44.01) + (0.734)(28.01) = 28.60 kg /kmol Sample calculations for CO 2 (i=2): h 2 = h f = 393,522 = 8942 M i 44.01 kj /kg ( ) Mi x 2 = y 2 = 0.125 44.01 M 28.60 = 0.1924 v 2 = Ru T M i P = 8.314 298 44.01 101 = 0.557 m3 /kg If all of the water is vapor, the water partial pressure would be P H2O = y i P = 0.141(101) = 14.2 kpa Whoever, at T = 298K, the saturation pressure of the water is 3.17 kpa (Table 3.1), so some fraction of the water will be liquid. The quality of the gas mixture is given in the Appendix: ( 1 X = y H2O X = 0.197 ) ( ) 1 P 1 1 = P sat ( 1 0.141 1 ) ( 101 3.17 1 ) 1 The enthalpy of vaporization h fg is 44.02/18.01 = 2444 kj/kg (Table 3.1) The term v fg is v g -v f = (1.362-0.001) = 1.361 m 3 /kg (Table 3.1) Therefore using equations (3.55) and (3.57) The enthalpy is given by: h = x 1 h 1 + x 2 h 2 + x 3 h 3 (1 X)x 1 h fg h = (0.0888)( 13,424) + (0.1924)( 8942) + 0 (1 0.197)(0.0888)(2444) h = 3087 kj /kg The specific volume is given by: v = x 1 v 1 + x 2 v 2 + x 3 v 3 (1 X)x 1 v fg v = (0.0888)(1.362) + (0.1924)(0.557) + (0.7189)(0.875) (1 0.197)(0.0888)(1.361) v = 0.760 m3 /kg

8 CHAPTER 3. FUEL, AIR, AND COMBUSTION THERMODYNAMICS 3.7) A four cylinder four stroke 2.8 L port injected spark ignition engine is running at 2000 rpm on a lean (φ =0.9) mixture of octane and standard air (101 kpa, 298 K) If the octane flow rate is 2.5 g/s, what is the mass of fuel entering each cylinder per cycle and the volumetric efficiency? a) The mass of fuel entering each cylinder per cycle for a four stroke engine ( ) ( ) ( ) ( ) 2 1 2 60 1 m f = ṁ f = 2.5 N 2000 4 n c m f = 3.75 10 2 g b) Since the engine is port injected e v = m a + m f ρ i v d = m f (AF + 1) ρ i v d = m f ( AFs φ + 1) ρ i v d From Table 3.5, the stoichiometric air-fuel ratio for octane is AF s = 15.03. Assume R = 0.287 ρ i = P RT = 101 (0.287)(298) = 1.18 kg /m 3 = 1180 g /m 3 Solving for the volumetric efficiency: η v = (3.75 10 2 ) ( 15.03 ( 0.9 + ) 1) (1180) η v = 0.80 2.8 10 3 4

9 3.8) An engine cylinder has a 90 mm bore and a 85 mm stroke, and contains air and residual gases at 350 K and 1 bar. If the engine is to operate on diesel fuel and run lean with an overall equivalence ratio of φ = 0.7, what is the mass of diesel fuel that needs to be injected during the compression stroke? (Assume R of the air-residual gas mixture is 0.29 kj/kg K). a) m = m a + m r We know that f = m r m Substituting we have Since m a = (1 f)m φ = F A F A s Substituting m f = φ(f A s )(m a ) = φ(f A s )(1 f)m Using the ideal gas law m f = P v d RT = P m f = 0.53 g ( π 4 RT ) b 2 s = 100 ( π 4 ) (0.09) 2 (0.085) (0.29)(350)(1000) From Table 3.5, AF s =14.30 or F A s =0.0699 The mass of injected diesel fuel is: m f = (0.7)(0.0699)(1 0.015)(0.53) m f = 2.5 10 2 g

10 CHAPTER 3. FUEL, AIR, AND COMBUSTION THERMODYNAMICS 3.9) Using the low temperature (T < 1000K) combustion equations, what are the composition, enthalpy, and entropy of the combustion products of methanol, CH 3 OH, at φ = 1.1, T = 1200 K, and P = 101 kpa? Compare with the results from the program ecp.m.

3.10) What are the mole fractions of CO 2, H 2 O, CO, N 2 and H 2 produced when methane (CH 4 ) is burned in rich conditions at φ = 1.1, T = 1000 K, and P = 101 kpa? 11

12 CHAPTER 3. FUEL, AIR, AND COMBUSTION THERMODYNAMICS 3.11) If a lean (φ = 0.8) mixture of methane CH 4 is burned at a temperature of 1500 K and pressure of 500 kpa, what are the mole fractions of the products, and the product enthalpy, entropy, and specific heat? Use the program ecp.m.

13 3.12) At what temperature does the saturation pressure P sat of an octane droplet equal 0.5 bar? At that temperature, what is the enthalpy of vaporization h fg? a) Antoine s equation is: [ log 10 (P sat ) = a b ] T + c Solving for T and using coefficients from Table 3.3 T = b a log 10 (P sat ) c Using coefficients from Table 3.3 1355.1 T = ( 63.633) = 375 K (octane) 4.0487 log 10 (0.5) 1739.6 T = ( 105.62) = 498 K (tetradecane) 4.1373 log 10 (0.5) This shows the greater volatility of octane relative to tetradecane b) The molar enthalpy of vaporization h fg is: h fg = Ae dt /Tc (1 TTc ) β Using coefficients from Table 3.4: ( 0.1834 375 h fg = 58.46 exp 568.8 ( 0.2965 498 h fg = 95.66 exp 694 ) ( 1 375 568.8 ) ( 1 498 694 ) 0.3324 = 36.2 MJ /kmol (octane) ) 0.2965 = 53.1 MJ /kmol (tetradecane) The octane value compares well with the value of 36.4 MJ /kmol in Table 3.2. requires about 47% more energy to vaporize. The tetradecane

14 CHAPTER 3. FUEL, AIR, AND COMBUSTION THERMODYNAMICS 3.13) Compare the enthalpy of vaporization h fg (MJ/kmol) of nitromethane, methanol, octane, and tetradecane at 400 K. a) The molar enthalpy of vaporization h fg is ( h fg = A exp α T ) ) β (1 TTc T c Using coefficients from Table 3.4 and molecular mass from Table 3.5 For Nitromethane: h fg = (53.33) exp h fg = 0.53 MJ /kg For Methanol: For Octane: h fg = (45.30) exp h fg = 0.95 MJ /kg h fg = (58.46) exp h fg = 0.30 MJ /kg For Tetradecane: h fg = (95.66) exp h fg = 0.31 MJ /kg ( 0.2732 400 ) ( 1 400 ) 0.2732 = 32.43 588 588 MJ /kmol = 32.43 61.04 ( ) ( 400 0.31 1 400 ) 0.4241 = 30.34 512.6 512.6 MJ /kmol = 30.34 32.04 ( ) ( 400 0.1834 1 400 ) 0.3324 = 34.31 568.8 568.8 MJ /kmol = 34.31 114.22 ( 0.2965 400 ) ( 1 400 ) 0.2965 = 62.50 694 694 MJ /kmol = 62.50 198.39 The charge cooling effect of the vaporization of methanol and nitromethane is 2-3 times that of octane and tetradecane on a per kg basis. The charge cooling produces greater volumetric efficiencies by increasing the density of the cylinder gases.

3.14) a.) If a rich (φ = 1.1) mixture of diesel fuel is burned at a temperature of 2000 K and pressure of 750 kpa, what are the mole fractions of the products, and the product enthalpy, entropy, specific volume, and specific heat? b.) Repeat the calculation for φ = 1.25. Discuss the effects of equivalence ratio. 15

16 CHAPTER 3. FUEL, AIR, AND COMBUSTION THERMODYNAMICS 3.15) Using the program ecp.m, plot the product equilibrium mole fractions as a function of equivalence ratio (0.5 < φ < 2) resulting from the combustion of methane at 5000 kpa and 2500 K.

17 3.16) Derive Equation (??) for the species mole fractions of a mixture of air and residual gas. a) The mixture m is composed of the residual mass m r and the premixed fuel-air m fa m = m f + m fa The residual mole fraction y r is y r = n r n fa + n r = 1 n fa n r + 1 Since the residual fraction f = mr /m or 1 f = m = m r + m fa = 1 + m fa m r m r m r m fa m r = 1 f 1 The mole ratio is n fa n r = m fa M fa Mr m r = m fa m r M M = ( ) 1 M f 1 M So y r = [1 + M M ( )] 1 1 f 1 The species mole fractions y i are y i = n i N = n i nfa n fa N + n i nr n r N = ( ni n fa ) y fa + Since the sum of the residual fractions must equal 1 y fa = 1 y r y i = n i n fa y i = n i n r ( ni n r ) y r So the species mole fractions accounting for both the residual gas and the inlet fuel- air y i = (1 y r ) y i + (y r ) y i

18 CHAPTER 3. FUEL, AIR, AND COMBUSTION THERMODYNAMICS 3.17) At what equivalence ratio for octane-air mixtures does the carbon to oxygen ratio of the system equal one? Why is this of interest? a) The combustion equation is C 8 H 18 + a s φ (O 2 + 3.76N 2 ) Products From Table 3.5, a s = 12.50 for octane. For every mole of octane, there are 8 carbon atoms and 2as /φ oxygen atoms. The carbon/oxygen ratio is: [C] [D] = 8 ( 2 ) a s φ So this ratio is equal to one, i.e. CO formation, φ = 2a s 8 = (2)(12.50) = 3.125 8 Therefore for φ > 3.125, there will be solid carbon in the products, since the carbon atoms are in excess of those used to form CO.

3.18) At what temperature is the concentration of H 2 a minimum for the combustion of gasoline and air at φ = 1.2 and 4500 kpa? What is that minimum value of H 2? 19

20 CHAPTER 3. FUEL, AIR, AND COMBUSTION THERMODYNAMICS 3.19) At what equivalence ratio is the concentration of OH a maximum for the combustion of diesel and air at T = 2500 K and 4500 kpa? What is that maximum value of OH?

3.20) At what temperature does the mole fraction of NO reach 0.010 for the equilibrium products resulting from the combustion of gasoline and air at φ = 1.0 and 5000 kpa? 21

22 CHAPTER 3. FUEL, AIR, AND COMBUSTION THERMODYNAMICS 3.21) At what temperature does the mole fraction of CO reach 0.080 for the equilibrium products resulting from the combustion of methane and air at φ = 1.1 and 3000 kpa?

3.22) What is the equilibrium and the frozen specific heat c p of the combustion products of gasoline at a pressure of 2000 kpa and temperature of 2000 K burned at a.) an equivalence ratio of 1.1, and b.) an equivalence ratio of 0.9? 23