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SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi Malaysia

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Page 1: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

SKMM 2413Thermodynamics I

Mohsin Mohd SiesFakulti Kejuruteraan Mekanikal, Universiti Teknologi Malaysia

Page 2: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

Synopsis

Thermodynamics is a basic science that deals withenergy. This course introduces students to the basicprinciples of thermodynamics. It will discuss basicconcepts and introduces the various forms of energyand energy transfer as well as properties of puresubstances. A general relation for the conservation ofenergy principle will be developed and applied toclosed systems and extended to open systems. Thesecond law of thermodynamics will be introduced andapplied to cycles, cyclic devices and processes.

Page 3: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

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THERMODYNAMICS AND ENERGY

• Thermodynamics: The science ofenergy.

• Energy: The ability to cause changes.• The name thermodynamics stems from

the Greek words therme (heat) anddynamis (power).

• Conservation of energy principle:During an interaction, energy can changefrom one form to another but the totalamount of energy remains constant.

• Energy cannot be created or destroyed.• The first law of thermodynamics: An

expression of the conservation of energyprinciple.

• The first law asserts that energy is athermodynamic property.

Page 4: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

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• The second law of thermodynamics:It asserts that energy has quality aswell as quantity, and actual processesoccur in the direction of decreasingquality of energy.

• Classical thermodynamics: Amacroscopic approach to the study ofthermodynamics that does not requirea knowledge of the behavior ofindividual particles.

• It provides a direct and easy way to thesolution of engineering problems and itis used in this text.

• Statistical thermodynamics: Amicroscopic approach, based on theaverage behavior of large groups ofindividual particles.

• It is used in this text only in thesupporting role.

Page 5: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

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Application Areas of Thermodynamics

All activities in nature involve some interaction betweenenergy and matter; thus, it is hard to imagine an area thatdoes not relate to thermodynamics in some manner.

Page 6: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

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Page 7: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi
Page 8: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

UNITS & DIMENSIONPhysical Quantity = Dimension

(length, mass, time, temperature, velocity, volume, etc)

Measurement of Dimension = Unit(meter, kg, seconds, …) SI system

Dimension Primary - length (m)mass (kg)time (s)temperature (K)

Secondary (Derived)e.g Volume = length3

Velocity = lengthtime

Page 9: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

Unit Addition- all terms must have the same dimension,unit, & factor (dimensional homogeneity)

Unit ConversionQuantities are multiplied with 1 (conversionfactor)

(Quantities unchanged, but units have changed)

Except temperature conversion since it involves addition

Page 10: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

SI Prefix

Page 11: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

Greek Alphabets

Capital Lowercase Name Pronunciation Capital Lowercase Name PronunciationΑ α ALPHA AL-fuh Ν ν NU NOOΒ β BETA BAY-tuh Ξ ξ XI KS-EYEΓ γ GAMMA GAM-uh Ο ο OMICRON OM-i-KRONΔ δ DELTA DEL-tuh Π π ϖ PI PIEΕ ε ϵ EPSILON EP-sil-on Ρ ρ RHO ROWΖ ζ ZETA ZAY-tuh Σ σ ς SIGMA SIG-muhΗ η ETA AY-tuh Τ τ TAU TAUΘ θ THETA THAY-tuh Υ υ UPSILON OOP-si-LONΙ ι IOTA eye-OH-tuh Φ ϕ φ PHI FEEΚ κ KAPPA KAP-uh Χ χ CHI K-EYEΛ λ LAMBDA LAM-duh Ψ ψ PSI SIGHΜ μ MU MYOO Ω ω OMEGA oh-MAY-guh

Page 12: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

System: A quantity of matter or a region in space chosen for study.

Surroundings: The mass or region outside the system

Boundary: The real or imaginary surface that separates thesystem from its surroundings.

The boundary of a system can be fixed or movable.Systems may be considered to be closed or open.

Page 13: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

Closed system (Control mass): A fixed amount of mass.Energy can cross the boundary, but no mass canOpen system (control volume): A properly selected region inspace.It usually encloses a device that involves mass flow such as acompressor, turbine, or nozzle.Both mass and energy can cross the boundary of a controlvolume.Control surface: The boundaries of a control volume. It can bereal or imaginary.

Page 14: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

Properties are characteristics of a system (e.g. Mass, volume,temperature, energy, pressure etc.)Types of property

ExtensiveThe value depends on the size of the system (additive)(Volume V, mass m, Energy E, Internal Energy U)

IntensiveThe value does not depend on the size of the system(not additive) (Temperature T, Pressure P)Specific Property (Independent of size)

Specific Property = (Extensive Property) / (Mass)ex. Specific Volume v, Specific Energy e

Property

e.g. Specific volume = Volume / mass

v [m3/kg] = V [m3] / m [kg]

Page 15: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

State

A state is described by the system propertiesat that instantIf even only 1 of the properties changed; thestate has changedIf all properties does not change with time; it iscalled steady stateIf the properties at two different times are thesame; both states are the same

Page 16: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

State Postulate

“The state of a simple, compressible system can becompletely described by knowing only 2 properties which areintensive and independent” (other properties can bedetermined from other relations)

State can be shown on a property diagram

Page 17: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

ProcessWhen state changes; the system has undergone a process

If several processes occurred in seriesuntil it reaches the initial condition; thesystem has undergone a cycle (netchange of any property = 0 after acycle)

Page 18: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

Constant Property ProcessWhen the value of a property is constant during the process

Page 19: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

Property (continued)

A quantity is a property iff (if and only if) thedifference between 2 states is not dependent onthe process between those states (point function).

If the difference of a function y is an exactdifferential (dy), that function is a thermodynamicproperty.

Work, heat depends on the path (process), andthus not an exact differential, and not a property(path function)

Page 20: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

SummaryWe are studying a system

Ex. Gas inside a piston-cylinder deviceGas = systemSurrounded by surroundingSeparated by a boundary (inside surface ofcylinder)

System has properties (T,p,v)Properties describe the state of the system (StatePostulate)State can be shown on a property diagramWhen state changes; the system underwent aprocessIf it returns to the initial state; the system underwent acycle

Page 21: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

Phase and Pure Substances

Phase - – a uniform amount of matter

Physical structure(solid, liquid, gas)

Chemical composition

Pure Substance – system with a uniformchemical composition

Page 22: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

Equilibrium

When there's no more change on any property- 4 things have to be in equilibrium

Thermal equilibrium

Phase equilibrium

Mechanical Equilibrium

Chemical equilibriumEquilibrium Process - System always in equilibrium

during process (process drawn assolid line on property diagram)

Quasistatic Process = quasiequilibrium (quasi = almost)

Page 23: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

TemperatureA fundamental quantity – a measure of molecular activity

Page 24: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

The Zeroth Law

Two systems in thermal equilibriumwith a third system are in thermalequilibrium with each other.

Page 25: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

PressurePressure: A normal force exerted by a fluid per unit area

Variation of pressure with depth∆ =

Page 26: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

Absolute, Gauge, and Vacuum Pressures

Page 27: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

Manometer & Barometer

Page 28: SKMM 2413 Thermodynamics I - fkm.utm.mymohsin/sme1413/01.english/chap01/01.intro.pdf · SKMM 2413 Thermodynamics I Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi

References

• Cengel, Boles, Thermodynamics, An Engineering Approach, 6th

Edition, McGraw Hill• Moran, Shapiro, Fundamentals of Engineering

Thermodynamics, John Wiley.• Sonntag, Van Wylen, Borgnakke, Fundamentals of

Thermodynamics, John Wiley.