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ENGR 2213 ENGR 2213 Thermodynamics Thermodynamics F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma
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ENGR 2213 Thermodynamics

Feb 23, 2016

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ENGR 2213 Thermodynamics. F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma. Syllabus. Instructor Dr. F. C. Lai (FH 218A) Phone: 325-1748, Fax: 325-1088, Email: [email protected] Office Hours: 14:00-15:00 MTWR or by appointment. Textbook - PowerPoint PPT Presentation
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Page 1: ENGR 2213  Thermodynamics

ENGR 2213 ThermodynamicsENGR 2213 Thermodynamics

F. C. LaiSchool of Aerospace and Mechanical EngineeringUniversity of Oklahoma

Page 2: ENGR 2213  Thermodynamics

SyllabusSyllabus

InstructorDr. F. C. Lai (FH 218A)Phone: 325-1748, Fax: 325-1088, Email: [email protected] Hours: 14:00-15:00 MTWR or by appointment

TextbookThermodynamics – An Engineering Approach by Y. A. Çengel and M. A. Boles, 4th edition, McGraw-Hill, 2002.

Page 3: ENGR 2213  Thermodynamics

Course OutlineCourse OutlineIntroduction (1+)● Basic Concepts● Properties

First Law (2-6)● Energy Analysis for Closed System● Energy Analysis for Control Volumes

Second Law (7-12)● Entropy● Exergy (Availability)

Page 4: ENGR 2213  Thermodynamics

Course OutlineCourse Outline

Power Systems (12-16)● Vapor Power Systems● Gas Power Systems

Page 5: ENGR 2213  Thermodynamics

GradeGrade

● Homework (8-10) 25%● Quizzes (3) 45% ● Final Exam 30%

Final grade (in absolute scale)85+ A75-84 B65-74 C55-64 D55- F

Page 6: ENGR 2213  Thermodynamics

IntroductionIntroduction

Thermo-dynamics heat force

● Energy → Engineers

● Properties of Matter → Scientists

Page 7: ENGR 2213  Thermodynamics

History of DevelopmentHistory of Development

~1700 Building a steam engine (T. Savery and T. Newcomen)

1849 First use of the term “Thermodynamics”(Lord Kelvin)

1859 First textbook of “Thermodynamics”(W. Rankine)

>1900 Become a mature science

Page 8: ENGR 2213  Thermodynamics

ApproachesApproaches

Macroscopic Approach (Classical Thermodynamics)

Microscopic Approach (Statistical Thermodynamics)

- is concerned with the overall behavior of a system- no model of the structure of matter at the molecular, atomic, and subatomic level is directly use

- is concerned directly with the structure of matter- characterize, by statistical means, the average behavior of the particles making up a system of interest and relate this information to the observed macroscopic behavior of the system

Page 9: ENGR 2213  Thermodynamics

DefinitionsDefinitions• System the subject of the analysis• Surroundings everything external to the

system• Boundary the surface that separates the

system from its surroundings

systemsurroundings

Page 10: ENGR 2213  Thermodynamics

DefinitionsDefinitions• System the subject of the analysis• Surroundings everything external to the

system• Boundary the surface that separates the

system from its surroundings

boundary

Page 11: ENGR 2213  Thermodynamics

SystemsSystems

Closed Systems

Control Volumes

- A fixed quantity of matter- There can be no transfer of mass across its boundary- Energy, in the form of heat or work, can cross the boundary- The volume of a closed system does not have to be fixed

- A fixed volume in space through which mass may flow- It usually enclose a device which involves mass flow such as a compressor, turbine, or nozzle

Page 12: ENGR 2213  Thermodynamics

SystemsSystems

Water HeaterPiston and Cylinder Assembly

Closed System

Page 13: ENGR 2213  Thermodynamics

SystemsSystems

Water HeaterPiston and Cylinder Assembly

Closed System Control Volume

Page 14: ENGR 2213  Thermodynamics

PropertiesProperties

Macroscopic characteristics of a system to which numerical values can be assigned.

Extensive Properties

Intensive Properties

Properties that their values depend on the size or extendof a system.

Properties that their values are independent of the size or extend of a system.

Examples: mass, volume

Examples: temperature, pressure

Page 15: ENGR 2213  Thermodynamics

PropertiesProperties

● Divide and Conquer● Rule of “Sum”

For a quantity, if its value for a system is the sum of itsvalues of each partition, then it is an extensive property.

Page 16: ENGR 2213  Thermodynamics

PropertiesProperties

● Divide and Conquer● Rule of “Sum”

For a quantity, if its value for a system is the sum of itsvalues of each partition, then it is an extensive property.

1 2 3 4

M = M1 + M2 + M3 + M4

Mass is an extensive property

Page 17: ENGR 2213  Thermodynamics

PropertiesProperties

● Divide and Conquer● Rule of “Sum”

For a quantity, if its value for a system is the sum of itsvalues of each partition, then it is an extensive property.

1 2 3 4

V = V1 + V2 + V3 + V4

Volume is an extensive property

Page 18: ENGR 2213  Thermodynamics

PropertiesProperties

● Divide and Conquer● Rule of “Sum”

For a quantity, if its value for a system is the sum of itsvalues of each partition, then it is an extensive property.

1 2 3 4

P = P1 = P2 = P3 = P4

Pressure is not an extensive property

Page 19: ENGR 2213  Thermodynamics

PropertiesProperties

● Divide and Conquer● Rule of “Sum”

For a quantity, if its value for a system is the sum of itsvalues of each partition, then it is an extensive property.

1 2 3 4

T = T1 = T2 = T3 = T4

Temperature is not an extensive property

Page 20: ENGR 2213  Thermodynamics

PropertiesProperties

Vvm

Specific Properties- Extensive properties per unit mass

Examples: specific volume

- A specific property is an intensive property

mV

density

Page 21: ENGR 2213  Thermodynamics

Basic ConceptsBasic ConceptsState

ProcessThe condition of a system as described by its properties

A transformation from one state to another

At a given state, each property has a definite value that isIndependent of how the system arrived at that state.

Page 22: ENGR 2213  Thermodynamics

Basic ConceptsBasic Concepts

The change in value of a property as the system is alteredfrom one state to another is determined solely by the twoend states and is independent of the particular way the change of state occurred.

A quantity is a property if, and only if, its change in valuebetween two states is independent of the process.

Page 23: ENGR 2213  Thermodynamics

Basic ConceptsBasic Concepts

Denver

Latitude Longitude ElevationDenver 39º 45’ 104º 52’ 5280’OKC 35º 24’ 97º 36’ 1285’

OKC

Page 24: ENGR 2213  Thermodynamics

Basic ConceptsBasic ConceptsPhaseA quantity of matter that is homogeneous throughout inboth chemical composition and physical structure.

Homogeneous in physical structure means that the Matter is all solid, all liquid, or all vapor (gas).

A system can contain one or more phases.For example: water and vapor 2 phases

Page 25: ENGR 2213  Thermodynamics

Basic ConceptsBasic ConceptsPhaseA quantity of matter that is homogeneous throughout inboth chemical composition and physical structure.

Homogeneous in physical structure means that the Matter is all solid, all liquid, or all vapor (gas).

A system can contain one or more phases.For example: water and vapor 2 phases

water and oil 2 phases

Page 26: ENGR 2213  Thermodynamics

Basic ConceptsBasic ConceptsPhaseA quantity of matter that is homogeneous throughout inboth chemical composition and physical structure.

Homogeneous in physical structure means that the Matter is all solid, all liquid, or all vapor (gas).

A system can contain one or more phases.For example: water and vapor 2 phases

water and oil 2 phases water and alcohol 1 phase

Page 27: ENGR 2213  Thermodynamics

Basic ConceptsBasic ConceptsPhaseA quantity of matter that is homogeneous throughout inboth chemical composition and physical structure.

Homogeneous in physical structure means that the Matter is all solid, all liquid, or all vapor (gas).

A system can contain one or more phases.For example: water and vapor 2 phases

water and oil 2 phases water and alcohol 1 phase oxygen and nitrogen 1 phase

Page 28: ENGR 2213  Thermodynamics

Basic ConceptsBasic ConceptsPure SubstanceOne that is uniform and invariable in chemical composition

A pure substance can exist in more than one phase

A uniform mixture of gases can be regarded as a puresubstance provided it remains a gas and does not reactchemically

Page 29: ENGR 2213  Thermodynamics

EquilibriumEquilibrium

Thermodynamic Equilibrium● Thermal Equilibrium● Mechanical Equilibrium● Phase Equilibrium● Chemical Equilibrium

A state of balance

In an equilibrium state, there are no unbalancedpotentials (driving forces) within the system.

Page 30: ENGR 2213  Thermodynamics

Thermodynamic EquilibriumThermodynamic Equilibrium

Mechanical Equilibrium

Thermal Equilibrium

● The pressure may vary within the system with elevation as a result of gravitational effect

● The system involves no temperature differentials● Temperature is uniform in the system

● No change in pressure at any point in the system

Page 31: ENGR 2213  Thermodynamics

Thermodynamic EquilibriumThermodynamic Equilibrium

Chemical Equilibrium

Phase Equilibrium

● No chemical reactions occur

● The mass of each phase remains the same

● Chemical composition does not change with time

Page 32: ENGR 2213  Thermodynamics

Basic ConceptsBasic ConceptsQuasi-Equilibrium ProcessA process that proceeds in such a manner that the system remains infinitesimally close to an equilibrium state at all times

A quasi-equilibrium process is an idealized process to approximate an actual process

Page 33: ENGR 2213  Thermodynamics

Basic ConceptsBasic ConceptsProcess PathThe series of equilibrium states through which a system passes during a processTo describe a process completely, one needs to specify the initial and final states of the process, as well as the path it follows

Steady StateProperties of the system does not change with time

CycleA sequence of processes that begins and ends at the same state