表面張力和接觸角英文課件

2008講稿-第6章Chapter6.SurfaceTensionand

ContactAngle6.1IntroductionSurfacetensionisaparametercanbeusedtocharacterizedpropertyofliquidsurface(interface)andmeasured.Contactanglecanbeusedmostlytocharacterizesurfacepropertyofasolidandmeasured.2008講稿-第6章FocusofthisChapterConcerningtheequilibriumbehaviorofinterfacesbetween“pure”phases;Definitionsandreasons;Lapalceequation,thepressureacrossacurvedinterface;Tousesurfacetensionandcontactangledeterminingwettingphenomenaofsolid.2008講稿-第6章6.2Surfacetension,surfaceworkand

surfacefreeenergySurfacetensionSurfacetension(γ)isaforcethatoperatesonasurfaceandactsperpendicular(垂直)andinwardfromtheboundariesofthesurface,tendingtodecrease

theareaoftheinterface.

F2008講稿-第6章γ=F/2L(1)Characteristics:Acontractile(收縮)force，tendstoshrink(收縮)thesurface;Aforceofperunitlength,(Nm-1ordynescm-1)；Atwo-dimensionalpressure;2008講稿-第6章（1）Reasonforproducing

surfacetensionAssumptionofvacantstateofsurface（表面層空位假說(shuō)）:（Bakker，Davies，F(xiàn)owkes，Ademson）Themoleculesinthesurfaceofliquidexchangeswiththemoleculesofitsvaporandtheliquid.2008講稿-第6章Basedonkineticmoleculartheoryofgases(氣體分子動(dòng)力學(xué)理論)andtheoryofdiffusioninliquids(液體擴(kuò)散理論),whentemperatureisin20?C：Exchangerateofmoleculesbetweensurfaceandvaporis:2.9×1020/s.cm2Exchangerateofmoleculesbetweensurfaceandliquidis:1.7×1025/s.cm22008講稿-第6章Inequilibriumthedistancebetweenthemoleculesonthesurfaceislargerthanthatinliquid,thereis“vacantposition”onthesurface.

Duetothedistancebetweenthemoleculesonthesurfaceislargerthanthatofthemoleculesinliquidthemoleculesinteractedattractivelyandinthestateoftension.Moleculesinliquid2008講稿-第6章ThedistancebetweenthemoleculesonsurfaceislargerthatpredicatedbythisassumptionisagreewiththedistancecalculatedbyPrigogineandSaragawithstatisticsmethodbasedonamodelofsurfacethermodynamics.Thermodynamicfunctionsofliquefiedargon(液氬)(85K)2008講稿-第6章（2）Mechanicalmodelofsurfacetension(表面張力的力學(xué)模型)Basedontheassumptionofvacantstateofsurface,surfacetensionofmattersisrelatedtotheforcesbetweenthemolecules.Surfacetension：Dispersionforce,Londonforce（d）(色散力);Hydrogenbonding(h)(氫鍵)Metallicbonding(m)(金屬鍵)Interactionofelectrons(π)(電子相互作用)Interactionofions(i)(離子相互作用)2008講稿-第6章SurfacetensiondefinedbyFowkes：

γ＝γd＋γh＋γm＋γπ＋γi

（6－1）Hydrocarbonliquids（H）：γH＝γHd

（6－2）Water（W）：γw＝γ

wd＋γ

wh

（6－3）Mercury(汞)(Hg)：

γHg＝γHgd＋γHgm

（6－4）Onlythedispersionforceexistinallmattersandthedistanceofthedispersionforceactonisthelongest(withinfewmolecules)。2008講稿-第6章Surfacetensionofmatters2008講稿-第6章（3）Surfacetensionandattractiveforce

Duetosurfacetensionisproducedbytheattractiveforcesbetweenmolecules,thevalueofinterfacetensionmeasurestheattractiveforcebetweenthemoleculesinliquidorthedifferenceoftheattractiveforce（?f）

betweenagasandliquid.Planesurface

γ－surfacetension

f－attractiveforce(liquid)f’-attractiveforce(gas)

?f=f－f’f’2008講稿-第6章γ－Surfacetensionf－Attractiveforceofthemoleculesonthesurface;f??－tangentialforceoff;f?－radialforceoff;Thevalueofsurfacetensionisrelatedtof??;Thetotaloff?istheextraforceactonthemoleculeinthesurfacetowardstothecenteroftheliquiddrop.Curvedsurface2008講稿-第6章（4）Directionofsurfacetension

Planesurface

：

Paralleltothesurface，contractileforce，tendstoshrinkthesurface

Curvedsurface

：2008講稿-第6章（5）SurfacetensionandtemperatureorpressureγandTT↑→γ↓（densityofgas↑，⊿f↓；distanceofmoleculesinliquid↑，⊿f↓）

γandPP↑→γ↓（someofmoleculesingasphasegointoliquid，⊿f↓；densityofgas↑，⊿f↓）2008講稿-第6章2．surfacework(表面功)Surfacetensionisacontractileforce,workcanbedonebytheforceundercertainconditions.

。

W＝2γLdx＝γdA

（6）Surfacework：Theworkdonebysurfacetensionwithreductionofsurfacearea.（J/m2）or（mJ/m2）2008講稿-第6章WhentheforceFmakethewirethoughdx,theworkdoneonthesystem,andtheworkequalstotheworkperunitarearequiredtoproduceanewsurface.FTwoequivalentinterpretationofγ：Forceperunitlengthofboundaryofthesurface;Energyperunitareaofthesurface.2008講稿-第6章3.surfacefreeenergy(表面自由能)Workdonebyreducingofsurfaceareapredictthatthesurfacehaveenergyandtheenergyisassurfacefreeenergy.Surfacefreeenergy：

Theenergyofthemoleculesonthesurfaceexcessintheenergyofthemoleculesinliquids.（mJ/m2）。

Surfacefreeenergyisan“excess”energy.2008講稿-第6章Fromthermodynamics,foraequilibriumsystemoftwophasesintheprocessofequilibriumtheworkdonebythesystemincludespressure-volumework(膨脹功),chemicalwork(化學(xué)功)andsurfacework,then：

dU＝TdS－PdV＋γdA＋（6－5）

2008講稿-第6章U－energyofthesystem；S－entropy(熵)；V－volume；T－temperature；P－pressure；μi－chemicalpotentialofi

component(成分)；

n－amountofsubstance(物質(zhì)的量)；

γ－surfacefreeenergy；

A－areaofsurface.2008講稿-第6章Surfacefreeenergyistheenergyofthesystemincreasedbyincreasingperunitareaofthesurfacewhenentropy,volumeandfractionsareconstant.Fromeq.(6-5)：2008講稿-第6章Basedondefinitionsofenthalpy(焓),freeenergy(自由能)andGibbsfreeenergy:

（6－6）（6－7）（6－8）2008講稿-第6章then：（6－9）（6－10）（6－11）Surfaceenergyisthechangeofenergyofthesystem,enthalpy,freeenergyandGibbsfreeenergybyincreasingperunitareaofthesurfaceundercertaincondition.2008講稿-第6章Whysmalldropsofliquidalwaysbechangedintoalargeonespontaneously?dG＝γdA，whenγisconstant，A↓→G↓2008講稿-第6章6.3Contactangleandwetting(潤(rùn)濕)WettingWettingisthedisplacement(置換)fromasurfaceofonefluid(流體)byanother.Wettinginvolvesthreephases,atleasttwoofwhichmustbefluids.Thewettingofagas(usuallyair)isdisplacedbyaliquidatthesurfaceofasolid.2008講稿-第6章Whenadrysubstance→wetsubstancetheenthalpy(焓)ofthesubstanceischanged.?Him＝Hwet－Hdry(6－12）?Him

–heatofimmersion(浸泡)?Him

<0，aprocessofreleasingheat(放熱).Airisdisplacedbyaliquidatthesurfaceofsolidspontaneously,?G<0.Enthalpyofwetting2008講稿-第6章Forasolidsurfaceofunitareaiswettedbyaliquidthefreeenergyischangedas

－?G＝γSA＋γLA－γSL＝WSL

（6－13）γSA－freeenergyoftheinterfacebetweenasolidandair;γLA－freeenergyoftheinterfacebetweenaliquidandair;γSL－freeenergyoftheinterfacebetweenasolidandaliquid;WSL－workofadhesion(粘附功)betweenasolidandaliquid.2008講稿-第6章Workofadhesionmeasurestheattractionbetweenthetwodifferentphases.Therefore,WSLcanbeusedtomeasurethedegreeofwetting.

γSAandγSLareunabletobemeasured.

Contactangle(θ)isusedformeasuringthedegreeofwetting.2008講稿-第6章Contactangle:Whenagas,aliquidandasolidareinequilibrium,theanglebetweentheinterfaceofsolidandliquidandatangentlineoftheinterfacebetweenthegasandliquidatthejunction(交點(diǎn))ofthethreephases(當(dāng)氣、液、固三相平衡時(shí)，在固－液－氣交點(diǎn)處作氣液界面的切線，此切線與固液界線的夾角)2.Contactangle2008講稿-第6章θ－Contactanglebetweenliquidandsolid;θ?－Contactanglebetweengasandsolid;θ＋θ?＝180?（6－14）θ>90?nowettableθ<90?wettable(潤(rùn)濕)θ＝0?wet(完全潤(rùn)濕)θ＝180?完全不潤(rùn)濕Contactangleismeasuredintheliquid.2008講稿-第6章Condition:1)Thesurfaceofasolidisperfectlysmooth;2)Thevapor,liquidandsolidareinequilibrium.γSA＝γSL＋γLAcosθ

（6－15）Taking（6－15）to（6－13）gives：

WSL＝γLA（1＋cosθ）（6－16）3.Young-Equatuin2008講稿-第6章Forθ＝0?，WSL＝2γLA（cohesionalworkofliquid,液體的內(nèi)聚功）θ＝180?，WSL＝0，完全不潤(rùn)濕。Noattractive(interaction)betweensolidandliquid.θ↓，WSL↑，θcanbeusedformeasuringdegreeofwetting.2008講稿-第6章（1）contamination(污染)ofsubstance

Forliquidiscontaminated→γLA↓，

ForsurfaceofsolidiscontaminatedγSAandγSL↓.親水表面4.Factorsaffectsthemeasurementofcontactangle親油表面2008講稿-第6章2）RoughnessofsolidsurfaceTherealsolidsurfaceisnotperfectlysmooth.

Roughnessfactor(粗糙度）（r）：

Ratioofthereal(真實(shí))surfaceareaofasolidtotheapparent(表觀)surfaceareaofthesolid.

r>12008講稿-第6章Forasolidsurfacewithroughnessfactorr,theYoungequationisgivenr（γSA－γSL）＝γLAcosθ?

（6－17）θ?－apparentcontactangle，comparing（6－17）with（6－15）gives

（6－18）2008講稿-第6章FromEq.(6-18)itwillbeA．Forθ<90?，θ?<θ，aroughsurfaceofasolidismorewettablethanasmoothsurfaceofthesolid.B．Forθ>90?，θ?

>θ，aroughsurfaceofasolidislesswettablethanasmoothsurfaceofthesolid.C．measurementofθisverydifficult.

θ↓

，errorsofmeasurement↑.2008講稿-第6章5.Advancing(前進(jìn))andReceding(后退)ContactangleAdvancingcontactangle(θa):

largervalueRecedingcontactangle(θr):

smallervalueBothadvancingandrecedingcontactanglesshouldbemeasured.2008講稿-第6章(θa)-

Thetilted(傾斜的)plateispushedintotheliquid.(θr)-

Thetiltedplateispulledoutfromtheliquid.2008講稿-第6章6.4Cohesion(內(nèi)聚),Adhesion(粘附)andSpreading(鋪展)1.CohesionNosurface→2A(orB)SurfacesCondition:

Oneunitofsurfaceisaffectedbytheprocess.Theshapeoftheaffectedareaisimmaterial(非物質(zhì)的).2008講稿-第6章Workofcohesion:TheworkrequiredtopullapartacolumnofliquidAapart.?G=2γA

=WAA(56)Itmeasurestheattractionbetweenthemoleculesoftwoportion.Surfacetensionmeasuresthefreeenergychangeinvolvedwhenmoleculesfromthebulkofasamplearemovedtothesurface.2008講稿-第6章2.Adhesion1ABInterface→1A+1BSurfacesDifferencebetweenthefinalandinitialfreeenergiesforthisprocessyields?G=WAB=γA+γB-γAB

(57)WABisworkofadhesionthatmeasurestheattractionbetweenthetwodifferentphases.2008講稿-第6章TheworkofadhesionbetweenasolidandaliquidphasemaybedefinedWSL＝γLA（1＋cosθ）(60)Forθ＝0?，

WSL＝2γLA

=WAAForθ＝180?，WSL＝0，theliquidistangenttothesolidandthereisnointeractionbetweenthephases.2008講稿-第6章3.Spreading?G=

γAB+γB-γA

(61)DifferencebetweenthefinalandinitialfreeenergiesforspreadingBoverA(symbolizedB/A)weobtainThenegativeof?GB/A

iscalledthespreadingCoefficientSB/A.2008講稿-第6章ForSB/A>0，

BspreadsfreelyoverAandwetsit.BycombiningEq.(56),(57)and(61)thespreadingcoefficientcanalsobewritten

SB/A=WAB-WBB

(62)IfWAB>WBB

theA-BinteractionissufficientlystrongtopromotethewettingofAbyB.2008講稿-第6章IfWAB<WBB

nowettingoccurs.SincetheworkrequiredtoovercometheattractionbetweentwoBmoleculesisnotcompensated(平衡)bytheattractionbetweenAandB.ForSB/A<0，BwillnotspreadoverA.

（《膠體化學(xué)基礎(chǔ)》135頁(yè)有誤）2008講稿-第6章6.5LaplaceEquationandCapillaryRiseTheLaplaceEquationObjective:Torelatethispressuredifferencetothecurvature(曲率)ofthesurface.Apressuredifferenceoperatesacrossacurvedinterface,andthegreaterpressureisontheconcave(凹)side.P1>P2.P1P2P12008講稿-第6章TheLaplaceEquation（29）Eq.(29)isgeneralandappliesequallywelltogeometricalbodieswithradiiofcurvaturethatareconstantovertheentiresurfaceortomoreintricate（復(fù)雜的）shapesforwhichtheRi’schangefromplacetoplaceonthesurface.2008講稿-第6章1．Forasphericalsurface，R1＝R2＝R，（30）2．

Foracylindricalsurface，R1＝∝，

(31)3．Foraplanarsurface，R1＝R2＝∝，?P＝0（32）

Thepressuresinbothsidesofthesurfaceareequal.2008講稿-第6章4．R1

andR2

↓，?P↑；

5．Foragasbubble,6.Forasaddle(馬鞍)shapedsurface,?P＝0，

7.Itmaybealiquidoragasatbothsidesofthesurface.

2008講稿-第6章

Thetotaloff?istheextraforceactonthesurfacetowardstotheconcave

sideoftheinterface.Duetothevalueof?Prelatetofandγrelatetof,therefore,γcanbeusedformeasuring

of

?P。Whythereisapressuredifferenceoperatesacrossacurvedinterface??P＝P?－PorP?＝P

＋?PPP’2008講稿-第6章Condition:Thewallofcapillaryiswettablebyaliquid.（1）彎曲液面壓差WhenacapillaryisjustpushedintowaterP1＝P2＝P3>P4Duetothepressureatpoint4islower，theliquidflowsfrompoint2towardpoint4andenterthecapillary.Atequilibrium:P5＝P1＝P2>P62.CapillaryRise2008講稿-第6章R－radiusofthecurvedsurface；

r－radiusofcapillary;Forr＝Rcosθ，then，

Thedifferenceofpressureacrossthecurvedinterfacepushliquidflowsintothecapillary.（6-19）2008講稿-第6章2．重力平衡（實(shí)驗(yàn)測(cè)定）Ifweimagine(設(shè)想)thesurfacetobe“hanging”fromthewallofthecapillaryandsupportedbytheverticalcomponent(γcosθ)ofthesurfacetension.《膠體化學(xué)基礎(chǔ)》24頁(yè)有誤“表面張力將流體拉入毛細(xì)管”，表面張力的分力與重力平衡。2008講稿-第6章《表面化學(xué)》，363頁(yè)P(yáng)ressuredifferenceacrossacurvedinterfaceas

（6－20）γLV－Surfacetensionbetweenliquidandvapor;r－Radiusofcapillary3．固－氣、固－液界面張力差2008講稿-第6章γSV－surfacetensionbetweensolidandvapor;γSL－surfacetensionbetweensolidandliquid；FromYoung-Equation（6－21）2008講稿-第6章?P＝2（γSV－γSL）/r（6－22）?PonlydependonthedifferenceofγSVandγSL，andnotrelatedtoγLV.ForγSV－γSL>0，capillaryrise；ForγSV－γSL<0，capillarydepression“毛細(xì)下降”。TakingEq.6-21intoEq.6-20gives2008講稿-第6章4．與表面張力反向力作用

《界面化學(xué)基礎(chǔ)》，15頁(yè)毛細(xì)管壁對(duì)液體的作用力將液體拉進(jìn)毛細(xì)管。Itimagine

f＝γ，andfoppositefromγ.f2008講稿-第6章Conclusionsforcapillaryrise：

1．ΔPor(γSV－γSL)isthedrivingforce;2．Foraspecifieds