MAE 431 ENERGY SYSTEMS I.

Similar documents
Thermodynamics EAS 204 Spring 2004 Class Month Day Chapter Topic Reading Due 1 January 12 M Introduction 2 14 W Chapter 1 Concepts Chapter 1 19 M MLK

4F-5 : Performance of an Ideal Gas Cycle 10 pts

Department of Civil Engineering & Applied Mechanics McGill University, Montreal, Quebec Canada

Fill in your name and ID No. in the space above. There should be 11 pages (including this page and the last page which is a formula page).

P=1 atm. vapor. liquid

Instructions: Show all work for complete credit. Work in symbols first, plugging in numbers and performing calculations last. / 26.

Chapter Outline 4/28/2014. P-V Work. P-V Work. Isolated, Closed and Open Systems. Exothermic and Endothermic Processes. E = q + w

2-18. (a) For mercury, (b) For water,

6-5. H 2 O 200 kpa 200 C Q. Entropy Changes of Pure Substances

Entropy. Chapter The Clausius Inequality and Entropy

Aircraft Performance - Drag

Study Guide Physics Pre-Comp 2013

ES201 - Examination 2 Winter Adams and Richards NAME BOX NUMBER

Control Volume (Eulerian Approach)

A review of A new determination of molecular dimensions by Albert Einstein

and for compressible flow

4-64. Review Problems

EXAMPLE: THERMAL DAMPING. work in air. sealed outlet

Lim f (x) e. Find the largest possible domain and its discontinuity points. Why is it discontinuous at those points (if any)?

Lecture 43: Aircraft Propulsion

Chapter 1 Notes Using Geography Skills

Phys101 Final Code: 1 Term: 132 Wednesday, May 21, 2014 Page: 1

Materials Engineering 272-C Fall 2001, Lecture 7 & 8 Fundamentals of Diffusion

UNIT 6 DETERMINATION OF FLASH AND FIRE POINT OF A LUBRICATING OIL BY OPEN CUP AND CLOSED CUP METHODS

Chemistry 114 First Hour Exam

Process Engineering Thermodynamics E (4 sp) Exam

Hooke s Law (Springs) DAVISSON. F A Deformed. F S is the spring force, in newtons (N) k is the spring constant, in N/m

CHAPTER 13 Temperature and Kinetic Theory. Units

bulk velocity through orifice,

Example 1. A robot has a mass of 60 kg. How much does that robot weigh sitting on the earth at sea level? Given: m. Find: Relationships: W

FINAL EXAM. ME 200 Thermodynamics I, Spring 2013 CIRCLE YOUR LECTURE BELOW:

Reference: 1. T. S. Gardner, C. R. Cantor, and J. J. Collins. Construction of a genetic toggle switch in Escherichia coli. Nature 403, (2000).

Thermodynamics and Equilibrium

FLUID FLOW FOR CHEMICAL ENGINEERING

Fundamental Concepts in Structural Plasticity

NGSS High School Physics Domain Model

Energy Inputs and Outputs

144 Chapter 12 States of Matter 2-9 BERNOULLI'S EFFECT. Answers to the Questions

Honors Physics Final Review Summary

i-clicker i-clicker Newton s Laws of Motion First Exam Coming Up! Components of Equation of Motion

convection coefficient. The different property values of water at 20 C are given by: u W/m K, h=8062 W/m K

Module 4: General Formulation of Electric Circuit Theory

Accelerated Chemistry POGIL: Half-life

Chapter 2. Coulomb s Law and Electric Field Intensity

Examiner: Dr. Mohamed Elsharnoby Time: 180 min. Attempt all the following questions Solve the following five questions, and assume any missing data

ChE 471: LECTURE 4 Fall 2003

Physics 231 Lecture 31

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

CHEM-443, Fall 2013, Section 010 Midterm 2 November 4, 2013

Q1. A string of length L is fixed at both ends. Which one of the following is NOT a possible wavelength for standing waves on this string?

Lecture 5: Equilibrium and Oscillations

Part One: Heat Changes and Thermochemistry. This aspect of Thermodynamics was dealt with in Chapter 6. (Review)

UNSTEADY, LAMINAR FLOW SIMULATIONS USING THE NONLINEAR DISTURBANCE EQUATIONS

Introduction to Thermodynamic Cycles Part 1 1 st Law of Thermodynamics and Gas Power Cycles

" 1 = # $H vap. Chapter 3 Problems

Types of Energy COMMON MISCONCEPTIONS CHEMICAL REACTIONS INVOLVE ENERGY

LINEAR MOMENTUM. Derivation of the Linear Momentum Equation. Newton s second law of motion for a system is. Momentum is mass times velocity.

Phys102 Final-061 Zero Version Coordinator: Nasser Wednesday, January 24, 2007 Page: 1

Kinetics of Particles. Chapter 3

Assume that the water in the nozzle is accelerated at a rate such that the frictional effect can be neglected.

Homework 1 AERE355 Fall 2017 Due 9/1(F) NOTE: If your solution does not adhere to the format described in the syllabus, it will be grade as zero.

Phy 212: General Physics II 1 Chapter 18 Worksheet 3/20/2008

Lecture 7 Further Development of Theory and Applications

KNOWN: Data are provided for a closed system undergoing a process involving work, heat transfer, change in elevation, and change in velocity.

Part 3 Introduction to statistical classification techniques

Comparison of hybrid ensemble-4dvar with EnKF and 4DVar for regional-scale data assimilation

Chapter 5: The First Law of Thermodynamics: Closed Systems

Fall 2013 Physics 172 Recitation 3 Momentum and Springs

Physics 1200 Mechanics, Kinematics, Fluids, Waves

Chapter 5: Diffusion (2)

CHEM Thermodynamics. Change in Gibbs Free Energy, G. Review. Gibbs Free Energy, G. Review

Q1. A) 48 m/s B) 17 m/s C) 22 m/s D) 66 m/s E) 53 m/s. Ans: = 84.0 Q2.

The First Law of Thermodynamics. By: Yidnekachew Messele

A) 0.77 N B) 0.24 N C) 0.63 N D) 0.31 N E) 0.86 N. v = ω k = 80 = 32 m/s. Ans: (32) 2 = 0.77 N

2015 Regional Physics Exam Solution Set

MAE 320 Thermodynamics HW 4 Assignment

Correlation and Statistical Characteristics of Turbulence Fronts in the Wakes of Hypervelocity Bodies

Compressibility Effects

Readings for this homework assignment and upcoming lectures

Physics 262/266. George Mason University. Prof. Paul So

To receive full credit all work must be clearly provided. Please use units in all answers.

Steady State Conduction

Equilibrium of Stress

More Tutorial at

Phys102 First Major-122 Zero Version Coordinator: Sunaidi Wednesday, March 06, 2013 Page: 1

Phy 213: General Physics III 6/14/2007 Chapter 28 Worksheet 1

Chapter 5. Mass and Energy Analysis of Control Volumes

PHYS 219 Spring semester Lecture 02: Coulomb s Law how point charges interact. Ron Reifenberger Birck Nanotechnology Center Purdue University

THERMAL TEST LEVELS & DURATIONS

EE247B/ME218: Introduction to MEMS Design Lecture 7m1: Lithography, Etching, & Doping CTN 2/6/18

Lecture 35: Vapor power systems, Rankine cycle

Introduction CHAPTER Prime Movers. 1.2 Sources of Energy

Chapter 3: Cluster Analysis

Thermodynamics: Gas Laws

Lecture 12: Chemical reaction equilibria

12. Shallow water equations with rotation Poincaré waves. Considering now motions with L<<R, we can write the equations of motion in

Solution to HW14 Fall-2002

Phys102 Second Major-102 Zero Version Coordinator: Al-Shukri Thursday, May 05, 2011 Page: 1

Three charges, all with a charge of 10 C are situated as shown (each grid line is separated by 1 meter).

CHAPTER 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES

Transcription:

MAE 431 ENERGY SYSTEMS I http://.eng.bffal.ed/crses/mae431 1

ENERGY SOURCES COAL Deep Mine Strip Mine NATURAL GAS Cnentinal Shale Gas OIL Cnentinal Shale Oil TYPE DISADVANTAGE ADVANTAGE Heat Energ Enirntal Damage Cheap, Abndant 12,000Bt/lb Occpatinal Danger Chemical Heat Energ 950 Bt/ft 3 Chemical Heat Energ 18,000 Bt/lb Chemical Well sealing Water clean p Difficlt in ransprtatin Ver Transprtable Limited Sppl Cheap Abndant Epensie Pliticall Sensitie GEOTHERMAl Heat Energ Limited Sppl N Fel Cst NUCLEAR FISSION Heat Energ Radiactie aste Fel cst Capital Cst FUSION Heat Energ Nt Cmmercial Lng Deelpment (50 r) Fel Cst L Radiatin Unlimited Sppl SOLAR Thermal Heat Energ Large Area Reqired N Fel Cst 200-250 Bt/ft 2 hr Unaailable Perids BIOFUELS Heat Energ Oil replacement HYDRO Ptential Limited Lcatins N Fel Cst WIND Kinetic Energ Limited Lcatins N Fel Cst > 30 mph reqired Unaailable Perids SOLAR Phtltaic Radiatin Energ Large Area Reqired N Fel Cst 200-250 Bt/ft 2 hr Unaailable Perids WAVE AND TIDE Kinetic Energ Limited Lcatins N Fel Cst Capital Cst ELECTRICITY? HYDROGEN?

ENERGY SYSTEMS ENERGY SOURCE TYPE ENERGY SYSTEMS COAL Deep Mine Strip Mine Heat Energ 12,000Bt/lb Steam Electric Heating Snfel NATURAL GAS Cnentinal Shale Gas OIL Cnentinal Shale Oil Heat Energ Gas Trbine Electric 950 Bt/ft 3 Gas Trbine Mechanical Cmbined Ccle Heating Heat Energ 18,000 Bt/lb Gasline Engine Diesel Engine Heating Aircraft Gas Trbinel GEOTHERMAl Heat Energ Steam Electric NUCLEAR FISSION Heat Energ Steam Electric FUSION Heat Energ Steam Electric SOLAR Thermal Heat Energ Steam Electric 200-250 Bt/ft 2 hr BIOFUELS Heat Energ Oil Sbstitte HYDRO Ptential Energ Electric WIND Kinetic Energ Electric > 30 mph reqired SOLAR Phtltaic Radiatin Energ Electric 200-250 Bt/ft 2 hr WAVE AND TIDE Kinetic Energ Electric

Gas Per Ccles Bratn Ccle Gas Trbine Aircraft - high elcit jet Transprtatin - mechanical per Statinar per - mechanical per Ott Ccle - spark ignitin engines Diesel engines - trcks, lcmties, statinar per Cmpressin Sstems - Prcess Indstr, Air tls Vapr Per Ccles Rankine Ccle steam and nclear plants Organic Ccle sstems Refrigeratin Ccles Vapr cmpressin - air cnditining, refrigeratin Heat Pmps Reerse Bratn Ccle - air cnditining, crgenics Nn-Reacting Mitres Gas Mitres Pschrmetrics Nn-Reacting Mitres Gas Mitres Pschrmetrics Reacting Mitres Cmbstin 4

Crse Smmar REVIEW OF THERMODYNAMICS Chapters 1-6, abt 3 eeks Chapter 1 Cncepts Thermdnamic sstem, prperties, state pint, prcess, ccle, heat and rk. Thermdnamic prblem sling techniqe. Chapter First La First La fr prcesses and ccles Chapter 3 Flid Prperties Real gases - steam, air, refrigerants tables Ideal gases, Eqatins f state First La in Clsed Sstems Chapter 4 Clsed Sstems First La in clsed Sstems Chapter Cntrl Vlmes Mass balance in Open Sstems First La in Open Sstems Chapter 6 Secnd La Statement and Crllaries Heat Engines Reersible engines and refrigeratrs Carnt Ccle Chapter 7 Entrp Secnd La and heat engines The Entrp prpert Isentrpic prcess Entrp change calclatin 5

Crse Smmar ENERGY SYSTEM TOPICS Chapters 7-13, abt 11 eeks Chapter 8 Eerg, Aailiabilit Aailabilit in Energ Sstems Eerg Chapter 15 Reacting Mitres Reactin mass balances. Reacting energ balances. Cmbstin Chapter 10 Vapr Per Ccles Rankine (steam per) reheat, sperheat and regeneratin ccles Chapter 9 Gas Per Ccles Bratn (gas trbine) ccle Ott (spark ignitin engine) ccle Diesel ccle Chapter 11 Refrigeratin Ccles Vapr Cmpressin Ccle Heat Pmps Reersed Bratn Ccle Chapter 12 Prpert Relatinships Using eqatins f state Maell Relatins Prpert Ealatin Chapter 13 Mitres Prperties f mitres. Chapter 14 Gas- Vapr Mitres Prperties f air ater apr mitres. Pschrmetrics 6

7

Q in W = W net tpt cmpressr trbine W Gas Generatr Per Trbine Aer-deriatie Gas Trbine 8

Frnas Hall J79-GE-8A Fighter Trbjet Engine First flight 1955, 17,000 bilt, replaced 1960 Cmpressr (right end), Cmbstr (red) Trbine (left end) 9

Frnas Hall J79-GE-8A Fighter Trbjet Engine Cmbstr (red) and Trbine Stages 10

Gas Trbine Technlgies Thermdnamics - prcess design, T, p and mass fl Aerdnamics - cmpressr and trbine blades Stress Analsis Vibratin Bearing and Lbricatin Sppl Rtrdnamics Manfactring Prcesses Mechanical Design Cntrls and instrmentatin Gas Trbine Engineering Tasks Design Reqirements Deelpment Design Deelpment Testing Manfactre Shp Testing Field Testing Installatin Maintenance Operatin Reamp Energ Sstems are nt all thermdnamics. Thermdnamics is the beginning f Energ Sstem design Prcess Design. This Crse: Thermdnamics f Energ Sstems Prcess Design f Energ Sstems 11

Thermdnamics Oerie Thermdnamics Thermdnamics is the std f the relatinship beteen all frms f Energ beginning histricall ith the relatinship beteen Heat and Wrk. Las f Thermdnamics ( fndamental bseratins) Mass Balance (shld be a la) Mass can nt be created r destred and is cnsered. First La (Energ Balance) Heat and rk are eqialent Prpert energ is defined Energ can change frm, can nt be destred, and is cnsered Secnd La Heat can nt be cnerted cmpletel t rk. Prpert entrp defined. Ideal and actal heat engine efficienc. 12

Thermdnamics Cncepts Thermdnamic Sstem Prperties State Pint Prcess Ccle Heat Wrk Energ First La - Energ Balance lead the analsis 13

WORK MASS HEAT Thermdnamic CONCEPTS Sstem Prperties State Pint Prcess Ccle Cntrl Vlme 3 Tpes f SYSTEMS Clsed Open Unstead 14

CLOSED THERMODYNAMIC SYSTEM NON FLOW SYSTEM A mass f material. Heat and Wrk can crss the sstem bndaries. Mass can nt. Heat Eamples: A clsed tank. A pistn clinder. Internal Cmbstin Clinder Wrk CONCEPTS Sstem Prperties State Pint Prcess Ccle 15

OPEN THERMODYNAMIC SYSTEM STEADY FLOW SYSTEM A fied regin in space. Mass, heat and rk can crss the sstem bndaries. Eamples: CONCEPTS Sstem Prperties State Pint Prcess Ccle trbine, cmpressrs,bilers, heat echangers Mass in Mass t Heat Wrk 16

UNSTEADY FLOW THERMODYNAMIC SYSTEM A ariable regin in space. Mass, heat and rk can crss the sstem bndaries CONCEPTS Sstem Prperties State Pint Prcess Ccle Eamples: A filling tank. An empting tank Pistn-Clinder Filling Heat Mass Wrk 17

18 Thermdnamic Prperties Temperatre Pressre Vlme Internal Energ Enthalp Entrp mass V,ft m,lbm/ft kg/m /lb ft m /kg, Ambient pressre Gage pressre Abslte pressre lb/in bar, atmspheres, kpa, 459.69 F R 273.15 C K 32. C 1.8 F R K, abslte, C, F, 3 3 3 3 3 3 2 = = = = = Vlme V Densit ρ SpecificVlme Pressre p Temperatre CONCEPTS Sstem Prperties State Pint Prcess Ccle

Thermdnamic Prperties SpecificInternalEnerg kj/kg, BTU/lb d = c c dt specifc heat at cnstant lme, 3 kg/jg, m /kg U InternalEnerg kj, BTU C, BTU/lbm F CONCEPTS Sstem Prperties State Pint Prcess Ccle h Specific Enthalp kj/kg, BTU/lbm h = p c p dh = c dt specific heat at cnstant pressre, H Enthalp kj, BTU H = m h s S Specific Entrp kj/ p S = m s Entrp kj/kg K C, kj/kg C, BTU/lbm F BTU/lbm F 19

THERMODYNAMIC STATE POINT Prperties are measred. Eqatins and mdels are fitted t the data reslting in : Tables f Prpert Vales Eqatins f State Cmpter prpert mdles T prperties define the state pint f a single phase flid. rdinate prpert (T,p,,,h,s) CONCEPTS Sstem Prperties State Pint Prcess Ccle One prpert defines the state pint f a mltiphase flid. absisa prpert 20

THERMODYNAMIC PROCESS A thermdnamic prcess is an interactin beteen a thermdnamic sstem and its srrndings hich reslts in a change in the state pint f the sstem Reersible Prcess A prcess is reersible if the state pints f all affected thermdnamic sstems, inclding the eternal sstem r srrndings, are retrned t their riginal state pint ales. Eamples: - mement f a frictinless pendlm - transfer f rk t ptential energ itht lss - mement f a frictinless spring CONCEPTS Sstem Prperties State Pint Prcess Ccle Irreersible Prcess A prcess hich can nt be reersed bringing all the affected thermdnamic prperties back t their riginal ales is irreersible. Eamples: - appling brakes t a ming heel - miing ht and cld ater - transfer f heat thrgh a finite temperatre difference Heat Wrk 21

Q ccle net W ccle net THERMODYNAMIC CYCLE A thermdnamic sstem nderges a ccle hen the sstem is sbjected t a series f prcesses and all f the state pint prperties f the sstem are retrned t their initial ales. = = ccle ccle Q W prcess prcess p CONCEPTS Sstem Prperties State Pint Prcess Ccle First δq = La δw initial pint is an ineact differential, a deriiatie that is path dependent. 22

Thermdnamic Prblem Sling Techniqe 1. Prblem Statement Carbn diide is cntained in a clinder ith a pistn. The carbn diide is cmpressed ith heat remal frm T1,p1 t T2,p2. The gas is then heated frm T2, p2 t T3, p3 at cnstant lme and then epanded itht heat transfer t the riginal state pint. 2. Schematic 3. Select Thermdnamic Sstem pen - clsed - cntrl lme a clsed thermdnamic sstem cmpsed t the mass f carbn diide in the clinder CO 2 W Q srrndings p p 4. Prpert Diagram state pints - prcesses - ccle Q T2,p2 T3,p3 T1,p1 5. Prpert Determinatin T2,p2 W Q T p h s W 1 2 3 6. Las f Thermdnamics Q=? W=? E=? material fls=? CONCEPTS Sstem Prperties State Pint Prcess Ccle 23

24 τ τ τ τ τ τ = ρ ρ τ τ τ ρ ρ ρ = ρ ρ τ τ τ ρ ρ ρ = ρ ρ τ τ τ ρ ρ ρ = ρ = T p T q q q T T T t T c ENERGY f p t f p t f p t directins,, MOMENTUM 0 t CONTINUITY p EQUATION SUMMARY - 3D, iscs, ariable densit, nstead