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M.BahramiENSC388(F09)IntroandBasicConcepts 1
BasicConceptsofThermodynamicsEverysciencehasitsownuniquevocabularyassociatedwithit.Precisedefinitionofbasicconcepts formsasound foundation fordevelopmentofascienceandpreventspossiblemisunderstandings.Carefulstudyoftheseconceptsisessentialforagoodunderstandingoftopicsinthermodynamics.ThermodynamicsandEnergyThermodynamicscanbedefinedas thestudyofenergy,energytransformationsand itsrelationtomatter.Theanalysisofthermalsystemsisachievedthroughtheapplicationofthe governing conservation equations, namely Conservation of Mass, Conservation ofEnergy (1st lawof thermodynamics), the2nd lawof thermodynamicsand thepropertyrelations.Energycanbeviewedastheabilitytocausechanges.First law of thermodynamics: one of the most fundamental laws of nature is theconservationofenergyprinciple. It simplystates thatduringan interaction,energycanchangefromoneformtoanotherbutthetotalamountofenergyremainsconstant.Second law of thermodynamics: energy has quality as well as quantity, and actualprocessesoccurinthedirectionofdecreasingqualityofenergy.Whenever there is an interaction between energy and matter, thermodynamics isinvolved. Some examples include heating and airconditioning systems, refrigerators,waterheaters,etc.DimensionsandUnitsAny physical quantity can be characterized by dimensions. The arbitrary magnitudesassignedtothedimensionsarecalledunits.Therearetwotypesofdimensions,primaryorfundamentalandsecondaryorderiveddimensions.Primarydimensionsare:mass,m;length,L;time,t;temperature,TSecondarydimensionsaretheonesthatcanbederivedfromprimarydimensionssuchas:velocity(m/s2),pressure(Pa=kg/m.s2).TherearetwounitsystemscurrentlyavailableSI(InternationalSystem)andUSCS(UnitedStatesCustomarySystem)orEnglishsystem.We,however,willuseSIunitsexclusivelyinthiscourse.TheSIunitsarebasedondecimal relationshipbetweenunits.TheprefixesusedtoexpressthemultiplesofthevariousunitsarelistedinTable11.
Table1:StandardprefixesinSIunits.MULTIPLE 1012 109 106 103 102 103 106 109 1012PREFIX tetra,T giga,G mega,M kilo,k centi,c mili,m micro, nano,n pico,p
M.BahramiENSC388(F09)IntroandBasicConcepts 2
Important note: in engineering all equationsmust be dimensionally homogenous. Thismeansthateveryterminanequationmusthavethesameunits.Itcanbeusedasasanitycheckforyoursolution.Example1:UnitConversionTheheatdissipationratedensityofanelectronicdeviceisreportedas10.72mW/mm2bythemanufacturer.ConvertthistoW/m2.
2
2
2 1072010001
1100072.10
mW
mWW
mmm
mmmW
ClosedandOpenSystemsAsystem isdefinedasaquantityofmatteroraregion inspacechosen forstudy. Themassorregionoutsidethesystemiscalledthesurroundings.
Fig.1:System,surroundings,andboundaryBoundary:therealorimaginarysurfacethatseparatesthesystemfromitssurroundings.Theboundariesofasystemcanbefixedormovable.Mathematically,theboundaryhaszerothickness,nomass,andnovolume.Closedsystemorcontrolmass:consistsofafixedamountofmass,andnomasscancrossitsboundary.But,energy inthe formofheatorwork,cancrosstheboundary,andthevolumeofaclosedsystemdoesnothavetobefixed.Opensystemorcontrolvolume:isaproperlyselectedregioninspace.Itusuallyenclosesadevicethat involvesmassflowsuchasacompressor.Bothmassandenergycancrosstheboundaryofacontrolvolume.Importantnote:somethermodynamicsrelationsthatareapplicabletoclosedandopensystemsaredifferent.Thus,itisextremelyimportanttorecognizethetypeofsystemwehavebeforestartanalyzingit.Isolated system:Aclosed system thatdoesnotcommunicatewith the surroundingsbyanymeans.Rigidsystem:Aclosedsystemthatcommunicateswiththesurroundingsbyheatonly.
SYSTEMBOUNDARY
SURROUNDINGS
M.BahramiENSC388(F09)IntroandBasicConcepts 3
Adiabatic system: A closed or open system that does not exchange energy with thesurroundingsbyheat.
Fig.2:Closedsystem,masscannotcrosstheboundaries,butenergycan.
Fig.3:Controlvolume,bothmassandenergycancrosstheboundaries.
EnergyInthermodynamics,wedealwithchangeofthetotalenergyonly.Thus,thetotalenergyofasystemcanbeassignedavalueofzeroatsomereferencepoint. Totalenergyofasystemhastwogroups:macroscopicandmicroscopic.Macroscopic forms of energy: forms of energy that a system posses as awholewithrespect to some outside reference frame, such as kinetic and potential energy. Themacroscopicenergyofasystem isrelatedtomotionandthe influenceofsomeexternaleffectssuchasgravity,magnetism,electricity,andsurfacetension.
energy
mass
CLOSEDSYSTEMm =const.
mass
energy
CONTROLVOLUME
M.BahramiENSC388(F09)IntroandBasicConcepts 4
Kinetic energy: energy that a system posses as a result of its relativemotionrelativetosomereferenceframe,KE
kJmVKE2
2
whereVisthevelocityofthesystemin(m/s). Potentialenergy:istheenergythatasystempossesasaresultofitselevationinagravitationalfield,PE
kJmgzPE wheregisthegravitationalaccelerationandzistheelevationofthecenterofgravityofthesystemrelativetosomearbitraryreferenceplane.
Microscopicformsofenergy:arethoserelatedtomolecularstructureofasystem.Theyareindependentofoutsidereferenceframes.Thesumofmicroscopicenergyiscalledtheinternalenergy,U.Thetotalenergyofasystemconsistsofthekinetic,potential,andinternalenergies:
kJmgzmVUPEKEUE 2
2
where the contributions of magnetic, electric, nuclear energy are neglected. Internalenergy isrelated to themolecularstructureand thedegreeofmolecularactivityand itmaybeviewedasthesumofthekineticandpotentialenergiesofmolecules.
Thesumof translational,vibrational,androtationalenergiesofmolecules is thekinetic energy of molecules, and it is also called the sensible energy. At highertemperatures,systemwillhavehighersensibleenergy.
Internalenergyassociatedwith thephaseofa system iscalled latentheat.Theintermolecularforcesarestrongestinsolidsandweakestingases.
The internal energy associated with the atomic bonds in a molecule is calledchemicalorbondenergy. The tremendousamountofenergyassociatedwith thebondswithinthenucleolusofatomitselfiscalledatomicenergy.
Energyinteractionswithaclosedsystemcanoccurviaheattransferandwork.
M.BahramiENSC388(F09)IntroandBasicConcepts 5
Fig.14:Formsofenergy.
M.BahramiENSC388(F09)IntroandBasicConcepts 6
PropertiesofaSystemAny characteristic of a system is called a property. In classical thermodynamics, thesubstanceisassumedtobeacontinuum,homogenousmatterwithnomicroscopicholes.Thisassumptionholdsaslongasthevolumes,andlengthscalesarelargewithrespecttotheintermolecularspacing.Intensiveproperties:arethosethatareindependentofthesize(mass)ofasystem,suchastemperature,pressure,anddensity.Theyarenotadditive.Extensive properties: values that are dependant on size of the system such asmass,volume,andtotalenergyU.Theyareadditive.
Generally,uppercaselettersareusedtodenoteextensiveproperties(exceptmassm), and lower case letters are used for intensive properties (except pressure P,temperatureT).
Extensive properties per unit mass are called specific properties, e.g. specificvolume(v=V/m).
Fig.15:Intensiveandextensivepropertiesofasystem.
StateandEquilibriumAtagivenstate,allthepropertiesofasystemhavefixedvalues.Thus,ifthevalueofevenonepropertychanges,thestatewillchangetodifferentone.Inanequilibriumstate,therearenounbalancedpotentials(ordrivingforces)withinthesystem. A system in equilibrium experiences no changes when it is isolated from itssurroundings.
Thermal equilibrium:when the temperature is the same throughout the entiresystem.
mVTP
0.5m0.5VTP
0.5m0.5VTP
extensiveproperties
intensiveproperties
M.BahramiENSC388(F09)IntroandBasicConcepts 7
Mechanicalequilibrium:whenthere isnochange inpressureatanypointofthesystem. However, the pressuremay varywithin the system due to gravitationaleffects.
Phaseequilibrium: inatwophasesystem,whenthemassofeachphasereachesanequilibriumlevel.
Chemical equilibrium: when the chemical composition of a system does notchangewithtime,i.e.,nochemicalreactionsoccur.
ProcessesandCyclesAnychangeasystemundergoesfromoneequilibriumstatetoanotheriscalledaprocess,andtheseriesofstatesthroughwhichasystempassesduringaprocessiscalledapath.
Fig.6:Tospecifyaprocess,initialandfinalstatesandpathmustbespecified.
Quasiequilibriumprocess: canbeviewedasa sufficiently slowprocess thatallows thesystemtoadjustitself internallyandremainsinfinitesimallyclosetoanequilibriumstateat all times. Quasiequilibrium process is an idealized process and is not a truerepresentationoftheactualprocess.Wemodelactualprocesseswithquasiequilibriumones.Moreover,theyserveasstandardstowhichactualprocessescanbecompared.Processdiagramsareusedtovisualizeprocesses.Notethattheprocesspath indicatesaseriesofequilibrium states,andwearenotable to specify the states foranonquasiequilibriumprocess.Prefixisoisusedtodesignateaprocessforwhichaparticularpropertyisconstant.
Isothermal:isaprocessduringwhichthetemperatureremainsconstant Isobaric:isaprocessduringwhichthepressureremainsconstant Isometric:isprocessduringwhichthespecificvolumeremainsconstant.
Asystemissaidtohaveundergoneacycleifitreturnstoitsinitialstateattheendoftheprocess.
State2
State1
Processpath
A
B
M.BahramiENSC388(F09)IntroandBasicConcepts 8
Fig.17:AfourprocesscycleinaPVdiagram.
The stateofasystem isdescribedby itsproperties.Thestateofasimplecompressiblesystemiscompletelyspecifiedbytwoindependent,intensiveproperties.A system is called simple compressible system in the absence of electrical,magnetic,gravitational,motion,andsurfacetensioneffects(externalforcefields).Independentproperties: twopropertiesare independent ifoneproperty canbevariedwhiletheotheroneisheldconstant.PressurePressureistheforceexertedbyafluidperunitarea.
PamN 2Area
ForcePressure Influids,gasesandliquids,wespeakofpressure;insolidsthisisstress.Forafluidatrest,thepressureatagivenpointisthesameinalldirections.
Fig.8:Pressureofafluidatrestincreaseswithdepth(duetoaddedweight),butconstant
inhorizontalplanes.
V
P
1
2
3
4
P(z)
z
Area=A
ghPAAhg
AmgP
P
Area
liquid ofWeight
h
A
M.BahramiENSC388(F09)IntroandBasicConcepts 9
Theactualpressureatagivenpositioniscalledtheabsolutepressure,anditismeasuredrelativetoabsolutevacuum.
gaugepressure=absolutepressureatmosphericpressure
atmabsatmvac
atmatmabsgauge
PPPPPPPPPP
Fig.9:Absolute,gauge,andvacuumpressures.
Inthermodynamicscalculations,alwaysuseabsolutepressure.Mostpressuremeasuringdevicesarecalibrated to read zero in theatmosphere (theymeasurePgauge orPvac).Beawareofwhatyouarereading!AdevicethatmeasurespressureusingacolumnofliquidiscalledaManometer.Thecrosssectionalareaofthetubeisnotimportant.Themanometermeasuresthegaugepressure.
Fig.10:Basicmanometer,P2=P1.
kPaghPP atm 1
Patm
Pgauge
Pabs
Absolute(vacuum)=0
P
Pvac
M.BahramiENSC388(F09)IntroandBasicConcepts 10
BourdonTubeisadevicethatmeasurespressureusingmechanicaldeformation.PressureTransducersaredevicesthatusepiezoelectricstomeasurepressure. veryaccurateandrobust canmeasurefrom106to105atm canmeasurePgaugeorPabs Barometerisadevicethatmeasuresatmosphericpressure.Itisamanometerwithanearvacuumononeend
Fig.11:Burdongauge.
Example2:PressureThepistonofacylinderpistondevicehasamassof60kgandacrosssectionalareaof0.04m2,asshown inFig.12.Thedepthof the liquid in thecylinder is1.8mandhasadensityof1558kg/m3.The localatmosphericpressure is0.97bar,andthegravitationalaccelerationis9.8m/s2.Determinethepressureatthebottomofthecylinder.Solution:thepressureatthebottomofthecylindercanbefoundfromthesummationoftheforcesduetoatmosphericpressure,pistonweight,andtheweightoftheliquidinthecylinder.
ghAmgPP
WWAPW
atmbottom
Pistonliquidatmbottom
M.BahramiENSC388(F09)IntroandBasicConcepts 11
bars
mNbar
smkgmN
msmmkgm
smkgbarPbottom
3918.1/10
1./1
/1
8.1/8.9/155804.0
/8.96097.0
252
2
232
2
Fig.12:Sketchforexample2.
TemperatureTemperatureisapointerforthedirectionofenergytransferasheat.
Fig.13:Heattransferoccursinthedirectionofhighertolowertemperature.
Whenthetemperaturesoftwobodiesarethesame,thermalequilibriumisreached.Theequalityoftemperatureistheonlyrequirementforthermalequilibrium.The0thlawofthermodynamics:statesthatiftwobodiesareinthermalequilibriumwithathirdbody,theyarealsointhermalequilibriumwitheachother.The0th lawmakesathermometerpossible.
A=0.04m2
h=1.8m
P=?
mPiston =60kgPatm=0.97bar
M.BahramiENSC388(F09)IntroandBasicConcepts 12
In accordancewith the 0th law, any system that possesses an equation of state thatrelates temperature T to other accurately measurable properties can be used as athermometere.g.anidealgasobeystheequationofstate:
mRPVT
ExperimentallyobtainedTemperatureScales:theCelsiusandFahrenheitscales,arebasedonthemeltingandboilingpointsofwater.Theyarealsocalledtwopointscales.Conventional thermometry depends onmaterial properties e.g.mercury expandswithtemperatureinarepeatableandpredictablewayThermodynamic Temperature Scales (independent of the material), the Kelvin andRankinescales,aredeterminedusingaconstantvolumegasthermometer.