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Notes on Difierential Geometry - CMU

NotesonDi erentialGeometrywithspecialemphasisonsur facesinR3 MarkusDesernoMay 3, 2004 Department of ChemistryandBiochemistry, UCLA,LosAngeles,CA90095-1569,USAMax-Plan ck-Institutf ur Polymerforschung,Ackermannweg 10,55128 Mainz,GermanyThesenotesareanattemptto summarizesomeof thekeymathe-maticalaspectsof di erentialgeometry, as theyapplyin particularto thegeometryof surfacesinR3. Thefocusis notonmathematicalrigorbutratheroncollect ingsomebitsandpiecesof theverypow-erfulmachineryof manifoldsand\post-Newtoniancalculus".Eve nthoughtheultimategoalof eleganceis a completecoordinatefreedescription,thisgo alis farfrombeingachievedhere|notbecausesuch a descriptiondoes notexistyet,butbecausetheauthoris farto thegeometricaspectsaretakenfromFrankel's book[9],onwhich thesenotesrelyheavily.

Hence, the components of the inverse metric are given by µ g11 g12 g21 g22 ¶ = 1 g µ g22 ¡g21 ¡g12 g11 ¶: (1.5) By virtue of Eqn. (1.4) the metric tensor can be used to raise and lower indices in tensor equations. Technically, \indices up or down" means that we are referring to components of tensors which live in the tangent space or the

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Transcription of Notes on Difierential Geometry - CMU

1 NotesonDi erentialGeometrywithspecialemphasisonsur facesinR3 MarkusDesernoMay 3, 2004 Department of ChemistryandBiochemistry, UCLA,LosAngeles,CA90095-1569,USAMax-Plan ck-Institutf ur Polymerforschung,Ackermannweg 10,55128 Mainz,GermanyThesenotesareanattemptto summarizesomeof thekeymathe-maticalaspectsof di erentialgeometry, as theyapplyin particularto thegeometryof surfacesinR3. Thefocusis notonmathematicalrigorbutratheroncollect ingsomebitsandpiecesof theverypow-erfulmachineryof manifoldsand\post-Newtoniancalculus".Eve nthoughtheultimategoalof eleganceis a completecoordinatefreedescription,thisgo alis farfrombeingachievedhere|notbecausesuch a descriptiondoes notexistyet,butbecausetheauthoris farto thegeometricaspectsaretakenfromFrankel's book[9],onwhich thesenotesrelyheavily.

2 For \classical"di erentialgeometryof curves andsurfacesKreyszigbook[14] hasalsobeentakenas a presentationvariesquitea greatdetail,othersareonlytoucheduponquic kly, mostlywiththeintent to indicateintowhich directiona particularsubjectmight be thetheory of nitions.. thesurface.. WeingartenandGauss.. conditions.. Identities.. nitionandproperties.. termsofrk.. expansion.. : Arclengthparameterization.. : Height is a functionof axialdistance.. : Axialdistanceis a functionof height .. a nitionof thevariation.

3 The rstfundamentalform.. of themetric.. thenormalvector.. thevolume.. theextrinsicgeometry.. problemsinvolvingthe .. ningproperty .. : Soap lmbetweentwo circles.. : Helicoid.. : Enneper'sminimalsurface.. 'sformula.. analysisfortheisoperimetricproblem.. equation.. of freecylindricalvesicles.. nitionandtransformationlaw.. coordinates.. erentialsandandpull-backs.. elds.. of Killing elds.. ,paralleltransport andcovariantdi .. of Levi-Civit a.. di erentiation.

4 :ThePoincar e plane.. elsymbols.. eldsof thePoincar e metric.. of a function,i. e., a scalar.. of a vector eld.. fora 1-form.. of a generaltensor eld.. :Liederivative of themetric.. problems62 Bibliography6431. Somefundamentalsof thetheory of thesurfaceLetUbe an(open)subsetofR2andde nethefunction~r: R2 U!R3(u1;u2)7!~r(u1;u2):( )We willassumethatallcomponents of thisfunctionaresu cientlyoftendi nefurtherthevectors1e ~r; :=@~r@u ;( )and~n:=e1 e2je1 e2j:( )If thee areeverywherelinearlyindependent2, themapping( )de nesa a di erentiablesubmanifoldofR3.

5 Thevectorse (~r) belongtoT~rS, thetangent spaceofSat~r, thisis why weusea di erent notationforthemthanthe\ordinary"vectorsf romR3. Notethatwhile~nis a unitvector,thee aregenerallynotof rstfundamentalformonthesurfaceSis de nedasgij:=ei ej:( )It is a secondranktensorandit is it is furthermore(everywhere)diagonal, thecoordinatesarecalledlocally denotedasgij, so thatwe havegijgjk= ki= 1ifi=k0ifi6=k;( )where kiis calledtheKroneckersymbol. Hence,thecomponents of theinversemetricaregivenby g11g12g21g22 =1g g22 g21 g12g11 :( )Byvirtueof Eqn.

6 ( )themetrictensorcanbe usedto raiseandlower indicesin ,\indicesupor down"meansthatwe arereferringto components of tensorswhich live in thetangent spaceor thecotangent space,respectively. It requirestheadditionalstructureof a metricin themanifoldin orderto de neanisomorphismbetweenthesetwo di erent of the rstfundamentalformis givenbyg:=detg jgj jgijj=12"ik"jlgijgkl;( )where"ikis thetwo-dimensionalantisymmetricLevi-Civi t a symbol"ik= i1 i2 k1 k2 = i1 k2 k1 i2; "ik="ik:1e =@~r=@u is @=@u (oreven shorter:@u ) thecanonicallocalcoordinatebasisbelongin gto requirement is thatthedi erential~r hasrank2 ( ).

7 4ntt SClocal tangent :Illustrationofthedef-initionofthenormal curvature n,Eqn.( ),andthegeodesiccurva-ture g, Eqn.( ).Theyareessen-tiallygiven by theprojectionof_~tontothelocalnormalvect orandonto thelocaltangent plane, 'is theanglebetweene1ande2, thenwe haveje1 e2j2=je1j2je2j2sin2'=g11g22(1 cos2') =g11g22 (e1 e2)2=g11g22 g12g21=g :Hence,we haveje1 e2j=pg somecurveCde nedonthesurfaceS, which goes throughsomepointP, at which thecurvehasthetangent vector~tandprincipalnormalvector~p=_~t= , andat which point thesurfacehasthenormalvector~n|seeas now have thefollowingtwo equations:~p ~n=cos#and_~t= ~p.

8 The rstde nestheangle#betweenthetwo unitvectors~nand~p, thesecondde nesthecurvatureof ,we obtain cos#=_~t ~n :( )If thecurve is parameterizedasui(s), we have_~t(s) = ~r(s) =@2@s2~r(s) =@@s ~r;i_ui =~r;ij_ui_uj+~r;i ui=ei;j_ui_uj+ei ui:Sinceei ~n= 0, we obtainfromthisandEqn.( ) cos#=_~t ~n= ei;j ~n _ui_uj:( )Theexpressionin bracketsis independent of thecurve anda property of is calledthesecondfundamentalform,andwe willtermitbij:bij:=ei;j ~n :( )Sinceei;j=ej;i, thesecondfundamentalformis symmetricin itstwo thesecondfundamentalformisfurthermoredia gonal, rstandsecondfundamentalformarediagonal,t hecoordinatelinesareorthogonalandtheyfor mlinesof curvature,i.

9 E., theylocallycoincidewiththeprincipaldirec tionsof curvature(seebelow).Di erentiatingtheobviousrelationei ~n= 0 withrespecttoujshowsthatei;j ~n+ei ~n;j= 0, fromwhich followsthatthesecondfundamentalformis alsogivenbybij:= ei ~n;j:( )Thisexpressionis usuallylessconvenient, sinceit involves thederivative of aunitvector,andthus thederivativeof square-root ,thecurvature of a curve at thepointPis partiallydueto thefactthatthecurve itselfiscurved,andpartiallybecausethesur faceis orderto somehow disentanglethesetwo e ects,it it usefulto de nethetwo conceptsnormalcurvatureandgeodesiccurvat ure.

10 We follow Kreyszig[14] in [14, paragraph60]fora moredetaileddiscussiononwhatthisimplies5 Thelefthandsideof Eqn.( )onlydependsonthedirectionof thecurve atP,i. e.~t, ,it is actuallya property of thesurface. It is calledthenormalcurvature nof thesurface in thedirection~t. If we performa reparameterizationof thecurve, we nd_ui= (dui=dt)(dt=ds) =u0i=s0, andfromthatwe nd: n:= cos#=biju0iu0jgiju0iu0j=bijduidujgijduid uj:( )Thenormalcurvatureis thereforetheratiobetweenthesecondandthe ( )showsthatthenormalcurvatureis a quadraticformof the_ui, or looselyspeakinga quadraticformof thetangent is thereforenotnecessaryto describe thecurvaturepropertiesof asurfaceat everypoint by givingallnormalcurvaturesin is enoughto know is naturalto ask,in which directionsthenormalcurvatureis ( )as bij ngij vivj=0.


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