Engineering Thermodynamics

Slides:



Advertisements
Similar presentations
ME 525: Combustion Lecture 3
Advertisements

CHEMICAL AND PHASE EQUILIBRIUM (1)
Course Outline Fundamentals and Combustion Systems Part I Chemical Equilibrium Chemical Kinetics Fuels Part II Flames Gas-Fired furnace combustion Premixed-charge.
Review of Chemical Thermodynamics Combustion MECH 6191 Department of Mechanical and Industrial Engineering Concordia University Lecture #1 Textbook: Introduction.
1st & 2nd Law Analysis for Combustion Process
Combustion and Power Generation
Advanced Thermodynamics Note 3 Heat Effects
Heat of Reaction 1st Law Analysis of Combustion Systems
Chapter 15 Chemical Reactions Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 7th edition by Yunus A. Çengel and.
Chapter 15 CHEMICAL REACTIONS
Chapter 16 Chemical and Phase Equilibrium Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition by Yunus.
Chapter 16: Chemical Equilibrium- General Concepts WHAT IS EQUILIBRIUM?
17 Chemical Equilibrium.
Equilibrium Basic Concepts Reversible reactions do not go to completion. –They can occur in either direction Chemical equilibrium exists when two opposing.
Chapter 14 Chemical reactions
1 General Concepts of Chemical Equilibrium. 2 In this chapter you will be introduced to basic equilibrium concepts and related calculations. The type.
Chapter 15 Chemical reactions.  Any material that can be burned to release thermal energy is called a fuel.  Most familiar fuels consist primarily of.
ME 475/675 Introduction to Combustion
Input + Generation = Output + Consumption
CHEMISTRY Matter and Change
Reacting Mixtures and Combustion
Mass Relationships in Chemical Reactions Chapter 3.
WCB/McGraw-Hill © The McGraw-Hill Companies, Inc.,1998 Thermodynamics Çengel Boles Third Edition 14 CHAPTER Chemical Reactions.
Daniel L. Reger Scott R. Goode David W. Ball Chapter 17 Chemical Thermodynamics.
Chapter 19 Chemical Thermodynamics. First Law of Thermodynamics Energy cannot be created nor destroyed. Therefore, the total energy of the universe is.
Reacting Mixtures and Combustion
CHAPTER 4 HEAT EFFECT. Consider the process of manufacturing ETHYLENE GLYCOL (an antifreeze agent) from ethylene : -Vaporization -Heating Ethylene (liquid)
CHAPTER 9 BALANCES ON REACTIVE PROCESSES By : Ms. Nor Helya Iman Bt Kamaludin 1 PTT 108: Mass and Energy Balances.
INTERNAL COMBUSTION ENGINES LECTURER PROF.Dr. DEMIR BAYKA.
PHYSICAL CHEMISTRY ERT 108 Semester II 2011/2012 Huzairy Hassan School of Bioprocess Engineering UniMAP.
ENERGY CONVERSION ES 832a Eric Savory Lecture 6 – Basics of combustion Department of Mechanical and Material Engineering.
ENERGY CONVERSION ES 832a Eric Savory Lecture 6 – Basics of combustion Department of Mechanical and Material Engineering.
AP Chapter 19.  Energy can not be created nor destroyed, only transferred between a system and the surroundings.  The energy in the universe is constant.
Chemistry 100 Chapter 19 Spontaneity of Chemical and Physical Processes: Thermodynamics.
Thermodynamics and Equilibrium. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–2 –We introduced the thermodynamic.
LECTURE 6 AOSC 434 AIR POLLUTION RUSSELL R. DICKERSON.
Department of Mechanical Engineering ME 322 – Mechanical Engineering Thermodynamics Review for Final Exam See also: Exam 1 prep Exam 2 prep Exam 3 prep.
Christian Madu, Ph.D. Collin College Lecture Presentation Chapter 4-1 Chemical Quantities and Aqueous Reactions.
Example from Lecture 6 A stoichiometric mixture of air and gaseous methane at 54 o C and 2 bar is buried in a 0.1 m 3 rigid vessel. The temperature of.
Energy Balance on Reactive Processes
Chemistry 231 Thermodynamics in Reacting Systems.
Power Plant Engineering
Review -1 School of Aerospace Engineering Copyright © by Jerry M. Seitzman. All rights reserved. AE/ME 6766 Combustion AE/ME 6766 Combustion:
Chemical Equilibrium By Doba Jackson, Ph.D.. Outline of Chpt 5 Gibbs Energy and Helmholtz Energy Gibbs energy of a reaction mixture (Chemical Potential)
CHEMICAL REACTION I am teaching Engineering Thermodynamics to a class of 75 undergraduate students. I plan to go through these slides in one 90-minute.
Chapter 20 Energy and Disorder.
Gibbs Free Energy Third Law of Thermodynamics Standard Molar Entropy (S°) Gibbs Free Energy Equation.
Chapter 9 Stoichiometry Test REVIEW SHEET
Finding and Using Molar Ratios The coefficients in a balanced chemical equation can be used to determine the relative number of molecules, formula units,
KANKESHWARI DEVI INSTITUTE OF TECHNOLOGY,JAMNAGAR a Presentation on “Equilibrium Thermodynamics and Kinetics” 5 th sem sub:- CET-II Prepared by
CHAPTER 15 CHEMICAL REACTIONS Lecture slides by Mehmet Kanoglu Copyright © The McGraw-Hill Education. Permission required for reproduction or display.
Chapter 9 Chemical Quantities.
ME 475/675 Introduction to Combustion
ME 475/675 Introduction to Combustion
Chapter Fourteen Chemical Equilibrium.
ME 475/675 Introduction to Combustion
Solution of Thermodynamics: Theory and applications
Unit 42: Heat Transfer and Combustion
Material Balances w/ Chemical Reactions
Gestão de Sistemas Energéticos 2016/2017
Gestão de Sistemas Energéticos 2016/2017
Chapter 5 Energy Balances with reaction.
Gas Stoichiometry.
Chapter 5 Energy Balances with reaction.
Chemical Equilibrium Equal but Opposite Reaction Rates
Gaseous Equilibrium – Chapter 12
Stoichiometry.
COMBUSTION THERMODYNAMICS DEEPA M S & VARUNA TANDON
Presentation transcript:

Engineering Thermodynamics Chapter 2. Fundamental Concepts in Understanding Bioenergy and Biobased Products Engineering Thermodynamics

Introduction •Thermodynamics essential to designing processing systems for biorenewable resources (Net energy output must be positive!!!) •Fundamental concepts include –Mass balances –Energy balances •These lectures not a substitute for a course in engineering thermodynamics

Kinds of Systems •Isolated system –neither mass nor energy enters the system •Closed system –mass does not enter or leave the system (no restriction on energy flow) •Open system –both mass and energy can flow through the system

Describing mass flow through an open system

Mass Balances for Combustion Processes The fuel-oxygen ratio (F/O) = mass of fuel per mass of oxygen (Sometime, F/O ratio could be written based on mole rather than mass.) The equivalence ratio () (F/O)stoichiometric is the Fuel-Oxygen ratio at which exactly all the available oxygen is used to burn the fuel completely The advantage of using equivalence ratio over fuel–oxidizer ratio is that it does not depend on the units being used.

Mass Balances for Combustion Processes (Continues) Example Consider a mixture of one mole of ethane (C2H6) and one mole of oxygen (O2). F/O ratio of this mixture based on the mass of fuel and O2 is: F/O ratio of this mixture based on the number of moles of fuel and O2 is: 2 2 1 1 2

To calculate the equivalence ratio, we need to first write out the stoichiometric reaction of ethane and oxygen Based on Mass: Based on Mole: (F/O)actual 0.938 1 (F/O)stoichiometric 30/112 = 0.268 1/(3.5) = 0.286 Equivalence Ratio 3.5 3.5

Mass Balances for Combustion Processes (Continues) The air in excess of the stoichiometric amount is called the excess air Actual Air Theoretical Air (%) = X 100 Stoichiometric Air Actual Air – Stoichiometric Air Excess Air (%) = X 100 Stoichiometric Air

Describing energy flow through an open system

Energy Balance for Open System *he or hi = specific enthalpy (energy / mass) *he or hi = specific molar enthalpy (energy / mole) *He or Hi = enthalpy (energy)

Energy Balance for Open System Within each inlet and outlet stream, we can have a multiple species. In this case, we need to add the enthalpy contribution from each and every species in the stream: . . - (Based on Mass) S mph S - mrh p p r r . . S nph S (Based on Mole) - nrh p p r r Hp Hr

Energy Balance for Open System Example:

Let us assume that 1 kmole/hr of biogas is produced by anaerobic digestion of animal waste consists of 60% of CH4 and 40% of CO2 (molar basis). The biogas reacts with 1.2 kmol/hr of O2 to form CO2 and H2O (no other products). Biogas + O2 T = To = 298K Q T = T2 = 1500K CO2 + H2O 0.6 CH4 + 0.4 CO2 + 1.2 O2  CO2 + 1.2 H2O

Specific Molar Enthalpy (kJ/kmol) We want to calculate Q under steady state condition for this example with following additional info. Specific Molar Enthalpy (kJ/kmol) T (K) CH4 O2 CO2 H2O 298 - 8,682 9,364 9,904 1500 71,078 57,999 The standard enthalpy of reaction (hR) is -890,330 kJ/kmol of CH4 at 298K. o Step #1: Do Energy Balance = - = H

Step #2: Calculate H Reactants H Products H HR (To) T To = 298K T2 = 1500K H = HR(To) + H = (-890,00)*(0.6) + [1*(71,078-9,364) + (1.2)*(57,999-9,904)] = -414,770 kJ/hr

Energy Balances For well-characterized fuels, standard enthalpies of reaction can be calculated from tabulations of specific enthalpies of formation, , of chemical compounds from their elements at a standard state: - nr and np are the stoichiometric coefficients for reactants and products of a chemical reaction h p ( r ( p r Example: Calculate the standard heat of reaction for the dehydrogenation of ethane: C2H6  C2H4 +H2

• Most biomass fuels are not well characterized in terms of their chemical constituents –Often simpler to perform calorimetric tests on biomass fuels to determine enthalpy of reaction

Thermodynamic efficiency • Every energy conversion process can be characterized by its thermodynamic efficiency

Chemical Equilibrium A B At equilibrium condition, a rate of forward reaction equals to a rate of reverse reaction = No Net Changes!!! Gibbs Free Energy and Entropy are two important thermodynamic properties in understanding chemical equilibrium

Chemical Equilibrium At the equilibrium condition, the equilibrium constant (K) can be defined. For a reaction involving ideal gases, the equilibrium constant based on partial pressures (Kp) can be expressed as:

Chemical Equilibrium ln If G > 0, then the reaction is not spontaneous. If G < 0, then the reaction is spontaneous. Everything in nature moves toward the equilibrium condition. The relationship between the Gibbs Free Energy and equilibrium condition can be written as: ln