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GasesTopicsinthislecture:KinetictheoryofidealgasesIdealgaslawPressureInternalenergyDegreesoffreedomMonatomicanddiatomicmoleculesTemperatureMaxwellBoltzmanndistributionofspeedsGasFillsthewholecontainerCanbecompressedKineticTheoryofGasesAssumptionsofkinetictheory
GascontainsmanymoleculesMoleculeshavenegligiblevolumeDirectionofmotionofmoleculesisrandomMoleculesexertnoforceoneachother,exceptwhencollideElasticcollisionsbetweenmoleculesandwithwallsAimingtomodelthebehaviourofaidealgaswithcomputersimulationsOurfirstunderstandingofgasmoleculeswasfromobservingdustparticlesmovingerratically.IdealGasLaw
R=molargasconstant=8.31JK-1mol-11Mole=6.02×1023particles=Avogadro’sNumber=NAP=pressure(Pa)V=volume(m3)T=temperature(K)n=numberofmoles1atm=1.013×105Pa1bar=105Pa1atm=1013millibar1Pa=1Nm-2FromexperimentsweseethatforfixedmassofgasIngeneralQuestion1Whatmassofoxygenisinthecylinderifithasavolumeof6litres,andisatapressureof10atmat20C?1atm=1.013x105PaMolarmassoxygen=32gNowPAUSEthevideoandtrytosolveQ1Question1Whatmassofoxygenisinthecylinderifithasavolumeof6litres,andisatapressureof10atmat20C?1atm=1.013x105PaMolarmassoxygen=32gHowdoeskinetictheoryexplainpressure?Pressureisduetocollisionsofmoleculeswiththewalls(andtheirchangeofmomentum).
PressureInitialmomentumofmolecule=+mvxFinalmomentumofmolecule=-mvxChangeofmomentumpermolecule=2mvx=densityInternalEnergyTheinternalenergyofagasisthesumthekineticandpotentialenergyofthemolecules.Inanidealgasthemoleculesdonotattracteachother,sotheyonlyhavekineticenergy.Whenheated,howistheenergystored?….asinternalenergyTranslationRotation3possibledegreesoffreedompermolecule3possibledegreesoffreedompermoleculeInternalEnergy–DegreesofFreedomEachwayinwhichasystemcanabsorbenergyiscalledadegreeoffreedomperdegreeoffreedomOnaverage,eachmoleculehasinternalenergyEquipartitiontheoremInternalEnergy–monatomicmoleculesU=internalenergy(J)k=Boltzmann’sconstant1.38×10-23(J/K)T=temperature(K)R=gasconstant=8.31Jmol-1K-1xyzE.g.He,Ne,Ar,Amonatomicmoleculehas3degreesoffreedomPermole,amonatomicgashas
but
Sointernalenergypermoleofmonatomicgas
InternalEnergy–diatomicmoleculesSointernalenergypermoleofdiatomicgas
Adiatomicmoleculehas5degreesoffreedom
E.g.H2,O2,N2,xyz
Generalequationforwholesampleofgas
Question2Determinetheinternalenergyof1moleofHelium(He)at20C2molesofhydrogen(H2)at27C
NowPAUSEthevideoandtrytosolveQ2
Question2
Determinetheinternalenergyof1moleofHelium(He)at20C(ii)2molesofhydrogen(H2)at27C
AveragekineticenergypermoleAveragekineticenergypermolecule
TemperatureMultiplyingbothsidesbyNARearranging:-Soweseethatrmsmeans-rootmeansquareM=molarmassTemperatureisproportionaltotheaveragemoleculartranslationalkineticenergy
Question3Theaveragespeedofairmoleculesinstillairatroomtemperatureisapproximately:-
Azero
B1mm/s(electrondriftspeedinmetal)
C2m/s(walkingspeed)
D30m/s(fastcar)
E500m/s(supersonicaeroplane)
F3×108m/s(speedoflight)NowPAUSEthevideoandtrytosolveQ3
Question3
Theaveragespeedofairmoleculesinstillairatroomtemperatureisapproximately:-
Azero
B1mm/s(electrondriftspeedinmetal)
C2m/s(walkingspeed)
D30m/s(fastcar)
E500m/s(supersonicaeroplane)
F3×108m/s(speedoflight)TheMaxwellBoltzmannDistributionJamesClerkMaxwell
1831-1879LudwigBoltzmann
1844-1906DistributionchangewithtemperatureVmax(speedofpeak)increaseswithtemperatureAreaundercurveremainsconstant,sopeaklowerFractionofMoleculesFractionofMoleculesAreaunderthecurveproportionaltototalnumberofmoleculesEvaporation-lossoffastmoleculesShapere-establishesitselfVmaxreducedwithreducedtemperatureAreaundercurvereducedassomemoleculeslostspeedFractionofMoleculesQuestion4Twodifferentsamplesofnitrogen,initiallyatdifferenttemperatures,aremixedtogether.ArethefollowingstatementsTRUEorFALSE?
(a)Themoleculeswillcollideandkineticenergywillbetransferreduntilallmoleculeshaveexactlythesameenergy.
(b)Beforemixingthespeedsofallthemoleculesofthehottergaswerehigherthanthoseofthecoolergas.
NowPAUSEthevideoandtrytosolveQ4Question4Twodifferentsamplesofnitrogen,initiallyatdifferenttemperatures,aremixedtogether.ArethefollowingstatementsTRUEorFALSE?
(a)Themoleculeswillcollideandkineticenergywillbetransferreduntilallmoleculeshaveexactlythesameenergy.
(b)Beforemixingthespeedsofallthemoleculesofthehottergaswerehigherthanthoseofthecoolergas.
SummaryIdealgasequationKinetictheoryisusedtomodelthebehaviourofanidealgas,intermofthemolecularbehaviourPressureisexplainedbythechangeinmomentumasthemolecu
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