CHM102 CarbonCompoundsandChemicalBonding: Valencebondtheory,shapesoforbitals; Hybridiza8on/LCAO,Molecularorbitaltheory; Hyperconjuga8on;Resonance;Tautomerismetc, (1hr) Whatdeterminestheshapeofmoecules? Lewisstructure CHM102-Aprl2016 2 ShapesallowmaximumdistancesbetweenatomsinABn molecules CHM102-Aprl2016 3 Canwepredicttheseshapesfromchemicalstructure? WhydomanyABnmoleculeshavesomanyshapes Valence-shellelectron-pairrepulsion(VSEPR)model CHM102-Aprl2016 4 Electronsinmoleculesbehaveliketheseballoons Op8mumgeometryexistsforeachnumberofballoons. Abondingpairofelectronsdefinesaregioninwhichtheelectronsaremost likelytobefound-theregionisanelectrondomain Nonbondingpair(orlonepair)ofelectrons -definesanelectrondomainthatislocatedprincipallyononeatom Eachnonbondingpair,singlebond,ormul4plebond producesasingleelectrondomainaroundthecentralatom inamolecule. CHM102-Aprl2016 5 VSEPRmodel:Electrondomainsarenega8vely chargedandthereforerepeloneanother. Thebestarrangementofagivennumberofelectrondomains istheonethatminimizestherepulsionsamongthem Twoelectrondomainsorientlinearly,threedomainsorientina trigonal-planarfashion,andfourorienttetrahedrally. Twoelectrondomainsorientina linearelectron-domaingeometry Neitherdomainisanonbondingpairofelectrons,the moleculargeometryisalsolinear CHM102-Aprl2016 6 CHM102-Aprl2016 7 Thesegeometriesareimportantbecause theyincludealltheshapesusuallyseenin moleculesorionsthatobeytheoctetrule CHM102-Aprl2016 8 EffectofNonbondingElectronsandMul8pleBondsonBond Angles Allthreehaveatetrahedralelectron-domaingeometry,buttheirbond anglesdifferslightly.Why? Bondanglesdecreaseasthenumberofnonbondingelectronpairs increases. • bondingpairofelectronsisa^ractedbybothnucleiofthebondedatoms, • nonbondingpairisa<ractedprimarilybyonlyonenucleus Nonbonding-lessnucleara^rac8on,itselectrondomainisspreadoutmorein spacethanistheelectrondomainforabondingpair Electrondomainsfornonbondingelectronpairsexertgreaterrepulsiveforceson adjacentelectrondomainsandtendtocompressbondangles. CHM102-Aprl2016 9 Rela8vevolumesoccupiedbybondingandnonbonding electrondomains Mul8plebondscontainahigherelectronic-chargedensitythansinglebonds, Mul8plebondsalsorepresentenlargedelectrondomains 3electrondomainssurroundthecentral atom,wemightexpectatrigonalplanar geometrywithbondangles120o Thedoublebond,however,seemstoact muchlikeanonbondingpairofelectrons, reducingthebondangleto111.4°: CHM102-Aprl2016 10 MoleculeswithExpandedValenceShells Atomsfromperiod3andbeyondmaybesurroundedbymorethanfourelectron pairs. Moleculeswith5or6electrondomainsaroundthecentralatomhavemolecular geometriesbasedoneitheratrigonal-bipyramidal(fivedomains)oroctahedral (sixdomains)electron-domaingeometry 5electrondomainsisthetrigonal bipyramid(twotrigonalpyramids sharingabase). Eachaxialdomainmakesanangle withanyequatorialdomain.Each equatorialdomainmakesa120° anglewitheitheroftheothertwo equatorialdomainsanda90°angle witheitheraxialdomain Inatrigonal-bipyramidalgeometry,therearetwotypesofposi8ons CHM102-Aprl2016 11 fortheouteratoms. Non-bondingdomain preferesequitorial ratherthanaxial?Why CHM102-Aprl2016 12 Non-bondingdomain preferesaxialratherthan axial?Why CHM102-Aprl2016 13 ShapesofLargerMolecules VSEPRmodelcanbeextendedtomorecomplexmolecules BondanglesaboutCand theOatomsdeviatefrom idealvaluesof120°and 109.5°-spa8aldemands ofmul8plebondsand nonbondingelectronpairs CHM102-Aprl2016 14 COVALENTBONDINGANDORBITALOVERLAP VSEPRmodel-meansforpredic8ngmoleculargeometriesbutdoesnot explainwhybondsexistbetweenatoms Useatomicorbitalstoexplainbondingandtoaccountformoleculargeometries? Valence-bondtheoryofchemicalbonding:Lewis’sno8onofelectron-pairbonds+ theideaofatomicorbitals • Bondingelectronpairsareconcentratedintheregionsbetweenatoms • Nonbondingelectronpairslieindirectedregionsofspace. Waysinwhichatomicorbitalscanmixwithoneanother Lewistheory:Covalentbondingbetweenatomssharingelectrons,concentrates electrondensitybetweenthenuclei CHM102-Aprl2016 15 Valence-bondtheory:visualizethebuildupofelectrondensity betweentwonuclei-whenavalenceatomicorbitalofoneatom sharesspace,oroverlaps,withavalenceatomicorbitalofanother atom CHM102-Aprl2016 16 HYBRIDORBITALS TheVSEPRmodel-goodjobatpredic8ngmolecularshape,thoughhas noobviousrela8onshiptothefillingandshapesofatomicorbitals. Basedontheshapesandorienta8onsofthe2sand2porbitalona carbonatom,itisnotobviouswhyaCH4moleculeshouldhavea tetrahedralgeometry. Atomicorbitalsaremathema8calfunc8onsthatcomefromthe quantummechanicalmodelforatomicstructure Atomicorbitalsonanatom(usuallythecentralatom)mixtoformnew orbitalscalledhybridorbitals.Theshapeofanyhybridorbitalis differentfromtheshapesoftheoriginalatomicorbitals. Numberofhybridorbitalsonanatomequalsthenumberofatomic orbitalsthataremixed. CHM102-Aprl2016 17 BeF2 Accordingtothevalence-bondmodel,alineararrangementofelectrondomains CHM102-Aprl2016 18 impliessphybridiza4on Forma8onofsp2hybridorbitals CHM102-Aprl2016 19 Forma8onofsp3hybridorbitals CHM102-Aprl2016 20 Hybridiza8onwithnonbondingpairsofelectrons .. H-O-H .. CHM102-Aprl2016 21 Carbon Hybridizations Unhybridized ↑↓ ↑ ↑ 2p 2s sp hybridized ↑ ↑ ↑ 2sp ↑ 2p sp2 hybridized ↑ ↑ ↑ 2sp2 sp3 hybridized ↑ ↑ ↑ ↑ 2p ↑ 3 2sp CHM102-Aprl2016 22 CHM102-Aprl2016 23 MULTIPLEBONDS CHM102-Aprl2016 24 FormaGonofandbondsinformaldehyde H2CO CHM102-Aprl2016 25 Multiple Bonds In triple bonds, as in acetylene, two sp orbitals form a σ bond between the carbons, and two pairs of p orbitals overlap in π fashion to form the two π bonds. ResonanceStructures,Delocaliza8on,andπ Bonding Bondingelectronsarelocalized-electronsareassociatedtotallywiththetwoatomsthat formthebond. Moleculesinvolvingmoreπ bonds? Eachcarbonissurroundedbythreeatomsat 120oangles,theappropriatehybridsetissp2 SixlocalizedC-Cσbonds SixlocalizedC-Hσbondsfromthe sp2hybridorbitals Eachunhybridized2porbitalis occupiedbyoneelectron,leaving sixelectronstobeaccountedfor bypbonding CHM102-Aprl2016 Theπbondsformedfrom overlapoftheunhybridized2p orbitalsonthesixcarbonatoms. 27 Delocalized πbondsinbenzene Delocaliza8onoftheelectronsinitsπbondsgivesbenzeneaspecialstability. Delocaliza8onofbondsisalsoresponsibleforthecolorofmanyorganic molecules. Op8maloverlapoftheunhybridizedporbitals-alltheatomsinvolvedina delocalizedπbondingnetworkshouldlieinthesameplane. Restric8onimpartsacertainrigiditytothemoleculethatisabsentinmolecules containingonlyσbonds CHM102-Aprl2016 28 Electron-domaingeometryatnitrogenis trigonalplanar:sp2hybridiza8onatN ConstructthethreeN¬Oσ bondspresent ineachresonancestructure. Unhybridized2porbitalontheNatom canbeusedtomakeπ bonds. CHM102-Aprl2016 29 Rota8onabouttheC=Cdoublebondinethylenebreaksthe π bond Rodsaresensi8vetodimlight-usedinnightvision. Conesaresensi8vetocolors. Thetopsoftherodsandconescontainamolecule calledrhodopsin:protein,opsin,bondedtoareddish purplepigmentcalledre4nal. CHM102-Aprl2016 30 MOLECULARORBITALS Valence-bondtheoryandHybridatomicorbitals:fromLewis structurestora8onalizingtheobservedgeometriesofmoleculesin termsofatomicorbitals. Valence-bondmodel-doesnotexplainallaspectsofbonding forex,describingtheexcitedstatesofmolecules, Howmoleculesabsorblight,givingthemcolor? Moresophis8catedmodelcalledmolecularorbitaltheory Electronsinatomscanbedescribedbywavefunc8ons,whichwe callatomicorbitals. Molecularorbitaltheorydescribestheelectronsinmoleculesby usingspecificwavefunc8onscalledmolecularorbitals(MO) CHM102-Aprl2016 31 Molecular Orbital Theory • In MO theory, we apply Schrödinger’s wave equation to the molecule to calculate a set of molecular orbitals. • In this treatment, the electrons belong to the whole molecule—so the orbitals belong to the whole molecule. – delocalization CHM102-Aprl2016 32 LCAO • The simplest assumption starts with the atomic orbitals of the atoms adding together to make molecular orbitals. This is called the linear combination of atomic orbitals method. • Because the orbitals are wave functions, the waves can combine either constructively or destructively. CHM102-Aprl2016 33 Molecular Orbitals • When the wave functions combine constructively, the resulting molecular orbital has less energy than the original atomic orbitals and is called a bonding molecular orbital. – σ, π – most of the electron density between the nuclei • When the wave functions combine destructively, the resulting molecular orbital has more energy than the original atomic orbitals and is called an antibonding molecular orbital. – σ*, π* – most of the electron density outside the nuclei – nodes between nuclei CHM102-Aprl2016 34 Theoverlapof2atomicorbitals,leadsto2molecular orbitals Destruc4vecombina4on. Electrondensity iszero an8bondingmolecular orbital Electrondensitytobe moreorlesscanceledin thecentralregionwhere thetwooverlap. Greatestelectrondensity onoppositesidesofthe twonuclei. Electroninanan8bonding MOrepelledfromthe bondingregion,higher energy)lessstable Construc4vecombina4on:the bondingmolecularorbital. Energyoftheresul8ngMOis Lowerenergy,morestablethan lowerthantheenergyofthe CHM102-Aprl2016 twoatomicorbitals the1satomicorbitalofan isolatedhydrogenatom 35 H2 σ*An8bondingMO LUMO σbondingMO HOMO CHM102-Aprl2016 36 Molecularorbitalscanexplainstabilityofmolecules ElectrondensityinboththebondingMOandthean8bondingMOofH2iscentered abouttheinternuclearaxis-sigmamolecularorbitals(byanalogytoσbonds). Energy-leveldiagram EnergydecreaserealizedingoingfromHe • MOislowerinenergythanthe1s atomicorbitalstotheHebondingMOisoffset atomicorbitals bytheenergyincreaserealizedingoingfrom • H2moleculeismorestablethanthe theatomicorbitalstotheHean8bondingMO. twoseparateHatoms. CHM102-Aprl2016 37 He2isanunstablemolecule Bondorder Bondorderof1representsasinglebond, Bondorderof2representsadoublebond, Bondorderof3representsatriplebond. MOtheoryalsotreatsmoleculeswithoddnumberofelectrons, bondordersof1/2,,3/2or5/2arepossible. H2=1;He2=0 He2+? Forma8onofHe2+inthegasphase CHM102-Aprl2016 38 1.ThenumberofMOsformedequalsthenumberofatomic orbitalscombined. 2.Atomicorbitalscombinemosteffec8velywithotheratomic orbitalsofsimilarenergy. 3.Theeffec8venesswithwhichtwoatomicorbitalscombineis propor8onaltotheiroverlap.Astheoverlapincreases,the energyofthebondingMOisloweredandtheenergyofthe an4bondingMOisraised. 4.EachMOcanaccommodate,atmost,twoelectrons,with theirspinspaired(Pauliexclusionprinciple). 5.WhenMOsofthesameenergyarepopulated,oneelectron enterseachorbital(withthesamespin)beforespinpairing occurs(Hund’srule) CHM102-Aprl2016 39 MolecularOrbitalsfrom2pAtomicOrbitals Theelectrondensitylies alongtheinternuclearaxis, sotheyaremolecular orbitals:σ2pand:σ*2p 2porbitalsoverlapsideways andthusconcentrateelectron densityaboveandbelowthe internuclearaxis. MOsofthistypearecalledpi (Π)molecularorbitals CHM102-Aprl2016 40 Energy-leveldiagramforMOsofperiod2homonuclear diatomicmolecules. CHM102-Aprl2016 41 Effectofinterac8onof2sand2porbitals • The smaller p-block elements in the second period have a sizable interaction between the s and p orbitals. • This flips the order of the σ and π molecular orbitals in these elements. CHM102-Aprl2016 42 LUMO Thehighestoccupiedmolecular orbital(HOMO)istheMOof highestenergythathaselectrons init.Thelowestunoccupied molecularorbital(LUMO)isthe MOoflowestenergythatdoes nothaveelectronsinit. HOMO HOMO–LUMOgap—isrelated totheminimumenergy neededtoexciteanelectronin themolecule. CHM102-Aprl2016 43 Hyperconjuga8on CHM102-Aprl2016 44 CHM102-Aprl2016 45 CHM102-Aprl2016 46 Tautomerism CHM102-Aprl2016 47
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