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Helical epitope of the group B meningococcal α(2-8)-linked sialic acid

polysaccharide

Brisson, Jean-Robert; Baumann, Herbert; Imberty, Anne; Pérez, Serge;

Jennings, Harold J.

(2)

Biochemistry

Helical

Epitope

of

the Group

B

Meningococcal

a(2-8)-Linked

Sialic

Acid

Polysaccharide*

Jean-Robert Brisson,1Herbert Baumann,1 Anne Imberty,****8

SergePérez,8 and

Harold

J. Jennings*’1 Institute

for

BiologicalSciences, NationalResearch Council

of

Canada,Ottawa, CanadaK1A OR6, andLaboratoire de

PhysicochimiedesMacromolécules, Instituí Nationaldela Recherche Agronomique, BP527, 44026NantesCédex, France Received December28, 1991; RevisedManuscriptReceivedMarch 11, 1992

abstract: The immunologicalproperties

of

the group Bmeningococcal

a(2-8)-linked

sialicacid poly-saccharide have been rationalized interms

of

a model where the randomcoil nature

of

the polymer can

bedescribed by thepresence

of

local helices. Theconformational versatility

of

the

aNeuAc(2-8)aNeuAc

linkagehasbeenexploredby

NMR

studiesat 600

MHz

in conjunction

with

potentialenergycalculations

for colominicacid,an

a(2-8)NeuAc

polymer,andthetrisaccharide

aNeuAc(2-8)aNeuAc(2-8)j8NeuAc.

Potentialenergy calculationswere usedto estimate theenergeticallyfavorable conformers andtodescribe thewide range

of

heliceswhichthe polymercan adopt. Nounique conformerwas found to satisfyall

NMR

constraints, andonly ensemble averaged nuclear Overhauser enhancements could correctly simulate the

experimentaldata. Conformationaldifferences between thepolymerandthe trisaccharide couldbebest

explainedinterms

of

slightchangesintherelative

distribution

of

conformersin solution.

Similar

helical parametersforthe

a(2-8)NeuAc

polymerand

poly(A)

were proposedasthebasisfor their cross-reactivity

toa monoclonalantibodyIgMNOV. The unusual length dependencyfor binding

of

oligosaccharide to group Bspecific antibodieswas postulated toarisefromthe recognition

of

ahigh-order local helixwithan extended

conformation whichwas not highly populatedin solution.

(jTroup

BNeisseriameningitidisandEscherichiacoliK1

are majorcauses ofmeningitis. Both bacteriahaveidentical capsular polysaccharides composedofa(2-8)-linkedsialic acid residues. Althoughvaccine developmenthasbeenhampered

by thepoorimmunogenicity ofthegroup B meningococcal polysaccharide inhumans,byN-propionylation ofits sialic acid residues, antibodies are produced which are both

bac-tericidal and protective [for reviews, see Jennings (1989, 1990)].

Thea(2-8)-linkedsialic acid homopolymerhasmany in-terestingimmunological propertieswhichhave beenextensively

studied. Thepresenceofa conformationalepitopewas

hy-pothesizedby Jennings et al. (1984) to explain theinability ofoligosaccharidesofup tofiveresiduestoinhibitthebinding

ofthegroup B polysaccharide toahomologoushorseantibody. Later,

it

was established that an unusually large deca-saccharide was required to bind or inhibit group B poly-saccharide specific antibodies (Jennings et al., 1985;Finne

&

Makela, 1985;Hayrinenet al., 1989). Thisisincontrastwith

aconventionalsequentialoligomerwhereonlyamaximum6 or 7 residues are necessary for binding (Rabat, 1960). Cross-reactivityofahumanmonoclonal antibody(IgMNOV)

withthe a(2-8)NeuAc‘ polymer, poly(A), and other

poly-nucleotideshas also been observed (Rabat et al., 1988). Various attemptshavebeenmade to relatethese immuno-logical properties to the three-dimensional structure ofthe antigen. Lindon et al. (1984), from

NMR

studies at 360

MHz,determined differencesintheorientationofthe exocyclic

chainsofthea(2-8)NeuAcanda(2-9)NeuAcpolysaccharides andinthe segmentalmotionofthe polysaccharides. Michon etal.(1987) determinedfrom

NMR

studiesat 500MHzthat the conformation ofthe linkagesofthe polysaccharideand fThisisNationalResearchCouncilofCanadaPublicationNo.32011.

Part ofthisworkwas made possiblethrough the France-Canada ex-changeprogram grantedtoJ.R.B.andfinancial support from INRA.

1NationalResearchCouncilofCanada. 8InstituíNationalde laRecherche

Agronomique.

shortoligosaccharideswere different. Yamasakiand Bacon (1991),fromaquantitativeanalysisof2DNOE’sat 500MHz

usingrigidmodels, suggestedthatthepolysaccharide adopts orderedhelical structures in solution. Inthe present paper, theconformational propertiesofcolominicacid,an

a(2-8)-NeuAc polymer, and the trisaccharide

aNeuAc(2-8)-aNeuAc(2-8)/3NeuAcwere evaluated by

NMR

studiesat 600

MHz,in conjunctionwithpotentialenergy calculations. The interpretationoftheNOE’swas based onamodelwhichallows

fortheinherent

flexibility

about thelinkages. The confor-mational versatilityofthemoleculewas estimated bypotential

energy calculations. The biological implications were

ra-tionalized in termsofamodel wheretherandom coil nature

ofapolysaccharidecan bedescribedbythe presenceoflocal helices (Perez

&

Vergelati, 1985).

Experimental

Procedures

Nuclear MagneticResonanceExperiments. Thecolominic acid polysaccharideand the trisaccharidewere preparedas

describedbefore(Michonetal., 1987),at concentrations

of

10-20mgin0.5mLof95%D20, 5% acetone-1/6,pH7,Na+ counterion. Samples were purgedwith helium gas. Upon storage atacoldtemperature,samplesinsolutionwere found to bestableformonths, withno signs ofdegradation. The

H3a and H3e resonances of the reducing terminus were

partiallydeuterated(>50%) afterseveralmonthsinsolution.

All experiments were performed on a Bruker AMX 600 spectrometer at 288 R. Foradditional temperature stability, thedeuteriumlockwas establishedon internalacetone-</6. No

significantchangesin chemicalshiftwere observed upon the

addition

of

acetone-d6. Forcolominicacid,pureabsorption

phasesensitive2DNOEexperimentswere doneinTPPImode

(Bodenhausen et al., 1984) withsix mixing timesof25, 50, 75, 100, 150, and 200 ms. The relaxation delay between

1

Abbreviations: COSY, correlation spectroscopy; NeuAc,

N-acetylneuraminicacid;NOE,nuclear Overhauser enhancement;NMR,

nuclear magneticresonance;TPPI, time-proportionalphase increments.

(3)

ConformationofMeningococcalB Polysaccharide Biochemistry, Vol. 31, No. 21, 1992 4997

TableI: MM2-MinimizedCoordinatesofaNeuAc-O-Me

atom X Y Z Cl 2.00350 -0.00013 1.42684 C2 1.42467 0.00407 0.00253 C3 1.85264 1.28886 -0.71271 C4 3.33580 1.26891 -1.05815 C5 3.63666 0.02645 -1.89345 C6 3.16028 -1.22252 -1.14587 C7 3.36974 -2.51478 -1.94809 C8 2.79059 -3.75974 -1.27483 C9 3.14742 -5.05286 -1.99458 CIO 5.59251 -0.31857 -3.37196 Cll 7.10639 -0.36067 -3.44988 Ola 1.35286 0.85734 2.23587 Olb 2.93208 -0.64255 1.83271 02 0.01649 -0.00037 0.00817 04 3.67387 2.43642 -1.80927 06 1.78881 -1.12261 -0.78919 07 2.77959 -2.38247 -3.24501 08 3.28173 -3.86537 0.06502 09 2.61127 -6.11483 -1.24381 010 4.90479 -0.55473 -4.34865 N5 5.06865 -0.02067 -2.13024 H3a 1.26995 1.39780 -1.65856 H3e 1.61658 2.18718 -0.09476 H4 3.95711 1.27566 -0.13132 H5 3.07491 0.12311 -2.85219 H6 3.76751 -1.31926 -0.21869 H7 4.46117 -2.67404 -2.11132 H8 1.67985 -3.67829 -1.20742 H9R 4.25246 -5.18468 -2.05049 H9S 2.71761 -5.10088 -3.02114 Hila 7.50134 -1.14014 -2.75920 Hllb 7.53118 0.62782 -3.16186 HI lc 7.44975 -0.60184 -4.48183 HN5 5.72929 0.09162 -1.36044 HOla 1.79198 0.79277 3.09998 H04 4.54535 2.33014 -2.15201 H07 3.35196 -1.87683 -3.79615 H08 4.20238 -3.66611 0.05735 H09 2.75650 -5.93429 -0.33581 CM2 -0.56945 -1.16138 0.57428 HM2a -0.19855 -1.33684 1.60824 HM2b -0.37743 -2.05165 -0.06578 HM2c -1.66970 -0.99793 0.61710

acquisitions was 6 s, and the sweep width was 2400 Hz. Matricesof512by 2048 pointswere recordedwitheightscans

pertxincrement. Transformationwasdoneusinga /2-shifted

sine-squaredbell

filter

in both dimensionand zero-fillingto

a square matrix

of

1024 X 1024 points for a final digital

resolutionof2.4Hz/point. Afirst-order polynomialbaseline correlationwas applied in the

fl

dimensionprior to volume integrationofthe cross-peaks. Theaverageoftheequivalent volumes aboveandbelowthe diagonalwas usedforanalysis.

All

data processingwas done usinguxnmr software provided

by Bruker. Steady-state ID NOE experimentson the

tri-saccharidewere doneasdescribed before(Michonet al., 1987). The spectrum

of

afewmilligrams ofcolominic acidwas

takenat various temperatures up to343K,inorder to observe the proton coupling constants. As described previously

(Michonet al., 1987),protonassignmentswere obtainedfrom

a COSY experiment. Spin simulations were done using

LAOCN5(QCPE) withftnmr (HareResearchInc.). Theerror on the coupling constantswas ± 0.3 Hz.

Calculations. The starting geometryof aNeuAcwas built

fromthecrystal structureoftheßsialicacidmethylglycoside (Flippen, 1973) afterproper settingofthe anomeric config-uration.

It

was thensubmitted to acomplete refinement

of

bond lengths,valence, and torsion angles byusing the

mo-lecular mechanics program MM2(87) (QCPE) (Burket

&

Allinger, 1982).

All

calculationswere done usingthe

mini-mized coordinatesforthemethylglycosideofaNeuAc (Table

I).

Foragivendisaccharide, the conformationalanalysiswas

evaluated usingthePFOSapproachwhich included the par-titioned contributions arisingfromvan derWaals interactions andtorsionaland exo-anomericpotential (Tvaroska

&

Perez, 1986). Rotational barriersof1.0and0.5kcal/molwere used for and

,

respectively. Noelectrostaticcontributionwas

considered. The ring geometrywas treatedasinvariant,and

hydroxylichydrogen atoms were not takenintoaccount. Four angles determine the linkage conformation for

aNeuAc(2-8)aNeuAc(h-a): =

(¿>06-¿>C2-¿>02-aC8),

= (¿>C2-¿02-tiC8-tiC7),

a>8 =

(07-C7-C8-08),

and 7 =

(06-C6-C7-07).

Theorientationofthe pendant groups for

Cl

andC9was definedby =

(Q6-C2-C1

-01

A) ando>9 =

(08-C8-C9-09). All

anglesare expressedindegrees. The

angles<vb 7, 8, and 9 were alwaysset the same forboth

residues. Thecv7anglewas setat60°,and separate mapswere

generatedfor 8 = 60°,

-60°,

and 180°

(g+,g",t). The

( , )

mapswere calculated in thefollowingway. Foragivenset of 7, w8values, theglycosidic torsionalangles and were

stepped in increments of 5° over the angular range which containedlowenergyminima,-120°to+240°for and40° to 220° for

.

At

eachpointofthisgrid search, the wj and

9 angleswere stepped in increments

of

20° over the whole angular range, andtheminimumenergy conformerwas

se-lected. Suchaprocedureallowedsevere steric constraintsto

berelievedbetweenthehydroxymethyl group atC9 and the carboxyl group at

Cl

across the glycosidic linkage.

All

the low energy conformers derivedfromthe analysisofsuch“rigid

potentialenergysurfaces”were refined using theMM2(87)

software. From alltheseminimizedconformers, theaverages

ofthe and<v8anglesforthethree staggeredtu8conformers

were takenand therigidmapswere calculated againusing

thesemean values(Table

II).

Theaverageglycosidicbridge

angleforbC2-b02-aCS of 117° was also used.

Helicesare customarilydescribedintermsofasetofhelical parameters, (n,h),withnbeing the numberofresiduesperturn

of

the helix and h being the translation

of

corresponding

residues along thehelixaxis. The parameternisderivedfrom the rotationangle (µ) about the helix axis per repeatunit,

wheren =

2 /µ.

Withsetvaluesofglycosidic valence angles andresidue geometry, these parameterscan becalculatedfor

TableII: MinimumEnergy Conformersfor<*NeuAc(2-8)a:NeuAc

E“ ^ OJg (Ug "1 <oi>6 n hc h/L

Gl+ 3.2 -45 130 55 70 138 -40 9.1 2.3 4.8 0.8 G2+ 0.0 75 100 55 70 138 -20 6.5 3.6 -3.2 -0.5 G3+ 2.9 -180 105 55 70 138 -40 6.7 11.3 5.7 0.9 Gl- 3.6 -50 120 60 -62 -162 -40 6.3 2.5 2.9 0.7 G2- 0.3 60 115 60 -62 78 -20 7.4 2.2 -4.2 -1.0 G3- 2.3 170 135 60 -62 -162 -40 6.9 2.8 -1.9 -0.5 T1 5.2 15 155 67 179 138 180 3.8 2.9 1.2 0.2 T2 1.0 80 160 67 179 98 180 4.7 3.0 '4.0 0.8 °Relative

(4)

Biochemistry, 31,

figure 1: Structureof aNeuAc(2-8)aNeuAcshowingthefour torsion

angleswhich determine thelinkage conformation with

(06-C6-C7-07) = 7 = 60° and(07-C7-C8-Q8) =

8 = 60°. The

ori-entation ofthe pendant groups at Cl and C9 isdefined by =

(06-C2-C1-01A)and 9 = (08-C8-C9-09),respectively.

any given value of the set of torsional angles (Sugeta

&

Miyazama,1967). Thelengthofthevirtualbond(L) between two adjacentlinking atoms,namely,

02

and

08,

represents themaximum ofthe possible extension. The quotient

h/L

yields the percentageoftotalextension. The chiralityisdefined by the signofh,positivefor right-handedhelices and negative

forleft-handedhelices.

The NOE was calculated using the complete relaxation

matrix, under the assumption of isotropic tumbling. The

steady-stateNOEwascalculatedasdescribedbefore (Brisson

&

Carver, 1983). The 2DNOEwas calculated accordingto Borgias and James(1988). Determinationofdistancesfrom 2D NOE data was done using the distance extrapolation method (Balejaet al., 1990). The ensemble averaged

NOE

was calculatedasdescribed byGummingandCarver (1987). For betterBoltzman weightingoftheNOE,apotentialenergy

mapwith Io increments in

( , )

was generatedfromthe 5° interval map using cubic spline interpolation. Only (r™6)

motional averaging was used. Averagingwas onlydonefor

( , ),

theo>7, 8, and 9 anglesbeingfixed. Foragiveno>7

and 8value, the

( , )

potentialenergy surfaceforwhich , and (ti9adopted minimumenergyconformers was used (see above) andtheaveragedNOEwas calculated separatelyfor

(ti9 = 60°,

-60°,

and 180°. This couldbe done becauseno

major interglycosidic NOE was observed on the H9

reso-nances. Therelativeenergyofconformerswithinawellwere

modifiedbyfirstdefiningacontourlevelwhichencompassed

alocalminimaandthen changing the energyoftheconformers at thegridpointswithinthewellbythesame amount. The relative population within a well was calculated using the Boltzmanndistributionon a 10 X 10 gridinterpolatedfrom a 5o X 5° grid.

Inorder to calculate theNOE,therotationalcorrelation timeofthe molecule mustbedetermined. It was estimated fromabest

fit

ofthecalculatedNOEtoH3a-H5and

H3e-H5 forvarious rigid conformers. Correlation timesof8 ns

and0.5nswere usedfor simulationoftheNOEfor colominic acid and the trisaccharide, respectively. The “standard deviation”,Sdev,fortheNOEwas calculatedusing7V(Sdev)2

=

( „

)2,

where

N

isthenumber

of

points. The n - h

plots for poly(A) were generated ina similar manner as described before (Yathindra & Sundaralingam, 1976) usingX-raycoordinates (Saenger etal., 1975). Ball andstickmodelswere generatedwiththeschakal program.

Calculationswere performedon Micro VAX 3200 and 3500.

Results

In order to understand the conformational behavior

of

«NeuAc(2-8)«NeuAc(Figure 1), thelinkage conformation

,

,

7, and 8, andtheorientation ofthe pendant groups mustbedetermined. Thepyranoseringadoptsawell-defined

figure 2: Potentialenergy contourmapfor aNeuAc(2-8)«NeuAc with( 7, 8)= (55°,70°)(A), (60°,-62°) (B),and(67°,179°) (C)

and(tijand 9 adoptingminimumenergy conformers. Withrespect

tothe globalminimumofeach section,the8,6,and10kcal/mollevels are drawnfor(A),(B),and(C),respectively. For(A),fromleftto right,three seperate wells,WG1+, WG2+,andWG3+,arethusdefined.

Similarly for (B),three wellsWG1",WG2™,andWG3'are defined. Localenergyminima (TableII)areindicated. Thehelical parameters

n (solid lines) andh(dotted line) are alsodisplayed. For poly(A)

(D),then- h

map and the energetically favoredhelices (dashed area)

are shown. The heliceswith (n,h) = (9,2.8Á) and (9,5.5Á)are

marked.

2C5conformation,andthe

NAc

groupat C5 adoptsaplanar

configuration withthe

H5-C5-N5-HN5

inthe trans con-figuration (Christian

&

Schultz, 1987).

PotentialEnergy Calculations. Potentialenergy calcula-tionswere performed in ordertoassess the

( , )

conforma-tional spaceforthestaggeredrotamers

of

8, with 7 fixed to theg+rotamer (Figure2). Thehelical parameters, ob-tained upon propagation of the molecule, are alsoplotted. Three

( , )

mapswere represented wherethe , and 9

ro-tamers were allowed to adoptminimum energyconformers

foreachsettingofthelinkage conformation. The 7 and 8 angleswere optimizedbymolecularmechanicscalculations. For the

( 7, 8)

=

(55°,70°) map(Figure2A), three major wells,WG1+, WG2+,andWG3+, whichencompassminima

Gl+,G2+, and G3+(Table

II)

are definedbythe8 kcal/mol

levelwithrespecttotheglobal minimum. Forthe ( 7, >8) =

(60°,-62°) map (Figure 2B), three separate wells, WG1", WG2~, andWG3“, couldbedefinedby the6 kcal/mollevel abovetheG2~conformer (Table

II).

The

( , )

energy map for((ti7,(ti8) = (67°,179°) mapswas more restricted,andonly the 10kcal/mollevelwithrespect tominimum T2 (Table

II)

isshownin Figure2C. Althoughother localminima could befoundwithinthese wells,onlytheareas defined bythese wellswere useful in interpreting theNOEresults. Relevant parameters forvarious low-energy conformers are givenin

TableII. Molecularmechanics calculationswere performed

forvariousconformerswithinthesewells (data not shown).

It was foundthattheseconformerswere stable,the linkage

anglesnot changingsignificantlyuponcompleteminimization.

Multipleorientationsofo>9were alsofavorable. The ,

ori-entationwas mostly restrictedto conformers around -170°

and-40°.

In orderto estimate the role

of

the charge, the average distance betweenthefouroxygen atomsforthecarboxylgroup

(5)

ConformationofMeningococcalB Polysaccharide Biochemistry, Vol. 31, No. 21, 1992 4999

Table III: Experimental 2DNOEVolumes‘ with75msof MixingTimeforColominicAcidandCalculated Relative NOE6

protons exp average' minima <G+> <G-> <T> Gl+ G2+ G3+ H3a-H3e 100 100 100 100 100 100 100 H3a-H8 9 8-11 8 2 32-41 2 28 H3e-H8 5 5-6 5 2 17-23 2 47 H3a-H7 3 3 2 2 4-6 2 74 H3e-H7 3 3 1 1 3 3 60 H5-H8 4 2-4 3 2 12-16 2 5 H3a-H5 24 22 22 22 24 22 30 H3e-H5 12 12 11 11 12-14 11 16 Sdev1' 1-2 2-3 4 10-15 4 34 H8-H6 28 26-33 5-6 7 30-42 26-30 40 H8-H7 30 20-24 27 9 22-31 19-22 31 H3a-H9“ 2 2-19 1-6 1 7-80 1 3 H3e-H9' 1 1-11 1-3 1 4-57 1 4 H7-H9' 11 3-4 6-18 4-19 5 3 4

Estimatederror = ±25%. 6TheH3a-H3eNOEissetto 100. ( 7, 8) forG+conformers = (55°,70°), for(G

> = (60°,-62°),andfor<T) = (67°,179°).

( , )

forGl+= (-45°,130°), forG2+= (75°,100°),forG3+= (180°, 105°). Significant

changesfor 9 = 60°,-60°,and 180° are shown. '

( , )

ensemble averagedNOE. Relativeenergies(in kilocaloriespermole)forwells WG1+, WG2+,andWG3+are 1.2:0:3andforwells

WG1", WG2“ andWG3"are 0.5:0:2. ‘'Standard deviationofthe fitfor sixmixing timesandforthefirst8volumesonly. The calculatedNOE

rangeforH9RandH9Sisalsoincluded.

5

figure 3: Partial NMRspectraof colominicacid at 600MHz and343K: (a)spinsimulated spectrum and (b) resolutionenhanced

spectrum.

less favored in solution due to the close proximity of the charged groups betweenadjacentresidues,whileforall the gauche conformers the carboxyl groups are further apart.

Colominic Acid. Colominic acid, which has a proton

spectrum identical tothat

of

thegroupBmeningococcal po-lysaccharide (data not shown), was used since

it

was more

readily available. Thechoiceofcounterion, thepH,andthe molecular weightfractionofthe polymerare importantfactors whichwere consideredin order togeta sampleas

homoge-neous aspossible anda stable samplewhich did not degrade

with time. The high molecular fraction of commercially available colominic acid (Na+ salt) was selected by gel

fil-tration. ThepH was adjusted to 7. Differentsampleswere

preparedwhichalways gave thesame spectra(Michonet al., 1987). Especially, the H8andH9resonances were resolved which permittedthe detectionof

NMR

parameterswhichwere

crucialinassessingthesolutionconformationofcolominic acid. In order to determine more accurately the vicinal proton

couplingconstants forcolominicacid, the spectrumwas

obtained at343

K

(Figure3).

All

multipletscouldberesolved andcorrectlyspinsimulatedto obtain accurate parameters. The proton coupling constants did not changewithtemperature (Lindonet al., 1984). Proton couplingconstantswere found to bethesame asthoseforresidue b

of

thetrisaccharideat 300K(Michonet al., 1987), exceptfor

/(H8,H9')

whichwas

5.5 Hzinstead of6.9 Hz.

The 2DNOEexperimentwithamixing timeof75ms, at

600MHz,and 288K, forcolominic acidisshownin Figure

4. Thevolumesthatcouldbeaccuratelymeasuredare given

7

figure 4: 2DNOEspectrum at 600MHzand 288K ofcolominic

acid. Themixing timewas 75ms. The IDspectrumisshownon

top along the

fl

axis.

in Table

III,

and some are plotted in Figure 5.

All

NOE

calculations were done using the coordinates for the di-saccharide(b-a). Adimercan be usedtosimulate theNOE’s

becausethe mostfavorable conformers formextended helices

whenpropagated (Figure2)with pitches(nh) greater than

5 Á. Hence, long-range interactions between nonadjacent residues

will

notbeimportant. For colominicacid, theNOE betweentwo protonswas taken asthesum

of

theinter-and intraresidue NOE ofthe equivalent pair. Forexample, the

H3a-H7 NOEwas thesum ofthe ¿H3a-¿>H7NOEandthe

¿>H3a-aH7 NOE. Forsome conformers, theinter- and in-traresiduecontributions were comparable.

TheNOE’s for

H3a-H5

and H3e-H5are dominated by

theintraresidueNOEonly. Fromthe2DNOEbuilduprates, using the distance extrapolation approximation (Table

IV),

theH3a-H5 andH3e-H5distanceswere foundto be2.5and

(6)

Biochemistry,

figure 5: 2DNOEbuildup rate for colominicacid. The experimental

volumesfor(H3a-H3e)/2

(·),

H3a-H5

( ),

H3e-H5

( ),

H3a-H8

(A), H3e-H8

( ),

H5-H8 (O),H3a-H7 (X),andH3e-H7(+)are shown. The

( , )

ensembleaveraged theoreticalNOE builduprates (solid lines) using thepotentialenergymapfor 7 =

55°, 8 = 70°

(Figure 2A) withanaltered relative energyforwells WG1+, WG2+, andWG3+of1.2:0:3kcal/moland the 9valuewhichgavethebest

fitare alsoplotted.

TableIV: DistancesforaNeuAcObtained from Minimized

Coordinates, from Distance Extrapolation0ofCalculated 2DNOE

Using ConformerGl+,andfromtheExperimental 2D NOE6 buildup

RateforColominicAcid

NOE

protons coordinates caled exptl

H3a-H3e 1.79

H3a-H5 2.51 2.5 2.5

H3e-H5 3.74 3.3 3.3

°a0 fromfit of y =

a0+ axx+ a2x2,where (y/r0)6 =

V/VQ, V0 =

H3a-H3evolume,r0= 1.79A, V=

cross-peakvolume, andx = mix-ing timesof25, 50, 75, 100, 150, and 200ms. ‘Estimatederror = 0.2

inagreementwiththe distanceof2.51

Á

calculatedfromthe coordinates ofTable I,adistanceof3.74

Á

isexpected for H3e-H5. However,

if

thebuildupratesare calculatedusing thecoordinatesofconformer

Gl+

andtheH3e-H5distance extrapolated from thecalculated volumes, avalue

of

3.3

Á

isobtained. Thereason for this discrepancy is thathigher

order effectsare neglectedinthe distance extrapolation method (Landy

&

Rao, 1989). Hence,inorder to accountforcorrect summation of the inter- and intraresidue NOE’s and the complete spin geometry,afullmatrixanalysiswas alwaysused.

TheNOEalso depends on allpairson interprotondistances

and thuson

,

,

7, 8,and 9. For motionalaveraging, the

NOEmustbeaveragedinacertain way dependingontherates ofinternal motion (Kessler etal., 1988). Inthiscaseonly

(r6)

averagingwas considered, since the modeofaveraging

will

notaffect anyoftheconclusions reachedin this study. The r"6 terms for a conformer were weighted according to the

Boltzmann distribution function.

TheNOE’swere analyzed usingamodel wherethe molecule

was allowed tosampleenergetically favored conformersover

( , )

with the 8 and 9 rotamers adopting staggered

con-formersonly. The 7 anglewas kept fixedtotheg+rotamer. Since,ingeneral,NOE’s thatwere highlydependentof and

were not greatly affected by thevalueof 9, thepotential energy map where 9 isallowed tofreelyrotate couldbeused

to calculatethe

( , )

ensemble averagedNOE for different

values

of

<u9. TheNOE’s for H3a-H8, H3e-H8, H3a-H7,

H3e-H7,andH5-H8 satisfied this conditionandthuscould

be usedtoassessthe

( , )

linkage conformation. The NOE’s

between

H3a-H9

andH3e-H9were notused becausethey

were highlydependenton 9, and theH9assignment toeither

figure 6: NOEconstraints mapofcolominic acidforamixing time of75ms. Thecalculatedrelative NOE’susing thefullrelaxation matrix, whichsatisfy theexperimental NOE’s (Table

III)

withan error boundof±25%are plottedas afunctionof

( , ),

with 7 =

55°, 8 = 70°. TheNOEconstraintsforH3a-H8 (-),H3e-H8

(|), H3a-H7(/),H3e-H7(\),andH5-H8(O) relative toH3a-H3eare

displayed. The mapsfor 9 = 60°,-60°,and 180°areoverlaid. The

8kcal/mollevelswhichdefine the threemajorenergy wellsWG1+, WG2 ,and WG3+(lefttoright) around theGl+,G2+, and G3+ confomers(Table

II)

are also shown.

H9Ror H9Swas ambiguous. Still,thesecalculatedNOE’s for differentvalues of<o9 were within the range of the

ex-perimentalones. Conversely, theNOE’sfor H8-H6, H8-H7, and

H7-H9

couldbeusedto determinetheorientationofthe exocyclic chainsincetheywere nothighlydependenton

( , ).

Theconformationofthe exocyclic chainwas determined fromthe protonvicinalcoupling constantswhicharedependent on thetorsionalangle

H-C-C-H

andfromNOE’s. Froma

spinsimulationofthe spectrum at343 K,

/(H6,H7)

and

/(H7,H8)

were found to be 1.0 and 2.3 Hz, respectively

(Figure 3). Also, the strongNOE for

H8-H6

and

H5-H7

(Figure4), indicatedthatthe 7 = 60°and

8 = 60° rotamers

were predominant in solution. Forthehydroxymethyl group at C9,

/(H8,H9)

and

/(H8,H9')

were 4.5and 5.5Hz,

indi-catingthatthestaggeredrotamersfor 9 were allaccessible. These resultsare similarto theones obtainedforthe

corre-spondinglinkage inthetrisaccharide (Michonetal., 1987). However, an NOE between the H7 and the H9 resonance

indicated thatthe other rotamers for 8 were also present.

Most probably,theg" rotamer was present dueto the small

/(H8,H7)

= 2.3Hzandthe large

H8-H7

NOE,whichcan

arisefrom bothgauche rotamers (Table

III).

FiveNOE’s couldbe used to evaluate the

( , )

linkage conformation,namely thoseforH3a-H8, H3e-H8, H3a-H7,

H3e-H7, and

H5-H8.

AnNOEconstraints mapwas

cal-culated to determine

if

allsetsofNOE’scan satisfyaunique

conformer. TheNOEwas calculatedforeachgridpointand

if

itsvalue fallswithinerror boundsofthe experimentalNOE, it was indicatedon themap. Forg+rotamers of 7 and 8, threemapswere calculatedforstaggered rotamers of 9 and overlaid. Nounique energetically favorable conformer satisfied

thefive experimentalNOEconstraints (Figure6). Similar resultswere obtainedfortheotherstaggered rotamer of 8. The experimental NOE’swere successfullysimulatedusing motionalaveragingover

( , )

(Table

III,

Figure5). Forthe

(7)

Conformation ofMeningococcal B Polysaccharide Biochemistry, Vol. 31, No. 21, 1992 5001

Table V: Experimental IDNOE" for aNeuAc(2-8)«NeuAc(2-8)/3NeuAc (c-b-a)andCalculated Relative NOE4

protonssat.obsd exptl

average' minima (G+> <G> <T> Gl+ G2+ G3+ cH3a-cH3e 100 100 100 100 100 100 100 cH3a-6H8 16 10-17 14 3 39-44 1 19-21 cH3a-6H6 3 2 1 4 6 1 12 cH3a-cH4 31 28 27 28 28 27 33 cH3a-cH5 53 55 57 59 51-54 56 78 cH3a-Z>H7 _d 3 2 2 5 2 80 cH3a-cH6 6 6 4-7 8 6 6 8 cH3a-cH7 3 4 3 3 4 4 6 cH3e-cH3a 100 100 100 100 100 100 100 cH3e-6H8 7 4-7 8 5 13-16 1 58-65 cH3e-6H6 4 1 1 6 2 1 22 cH3e-cH4 46 55-64 54 52 63-102 51 66 cH3e-cH5 21 22 21 22 20-26 21 23 cH3e-6H7 ud 4 1 2 3 5 55 cH3e-cH6 7 6-8 4-8 8 7-12 6 8 cH3e-cH7 -e 2 2 2 4 2 3 SdeV 4-6 4 5 9-19 6 40 6H8-6H7 100 100 100 100 100 100 100 6H8-6H6 114 102-106 12-23 71-87 108-122 104 240 6H8-6H3a 21 16-19 12-14 6 33-64 2 43 ¿>H8-6H3e 14 7 6-8 8 12-21 2 130 6H8-6H5 12 8 5 37-48 3 13

“Estimatederror = ±25%. 4ThereferenceNOEissetto 100. ( 7, 8) forG+conformers = (55°,70°), for<G) =

(60°,-62°),andfor (T) =

(67°,179°).

( , )

forGl+= (-45°,130ß), forG2+= (75°,100°),andforG3+= (180°,105°). Significant

changesfor , = 60°,-60°,and 180»

areshown. '

( , )

ensemble averagedNOE. Relativeenergies(in kilocaloriespermole) forwellsWG1+, WG2+,andWG3+are 0.4:0:3andforwells

WG1", WG2",are 0.5:0:2. ‘'ResonancescH5and6H7overlap. ‘AbsoluteNOE<1 ± 1. ^ForcH3aandcH3eNOE’s only.

7 = 55°, 8 = 70° energy surface, threemajorwells,WG1+,

WG2+,andWG3+, whichencompassconformers

Gl+,

G2+, and G3+can bedefined by the8kcal/mollevelwithrespect totheglobalminimumG2+ (Figure2A).

With

therelative energy for minima

Gl+,

G2+, and G3+ of 3:0:3 kcal/mol obtainedfromthe potential energy calculations, the relative

populationofwellWG1+was 99%,whiletheotherwells had

lessthan 1%occupancy. The

( , )

ensemble averagedNOE’s calculated using this distribution were the same as those calculated using the singleminimum conformerG2+, sincefor allconformerswithinwell WG2+, interglycosidic NOE’swere

small, compared tothoseforconformer

Gl+

or G3+(Table

III).

Hence, poor agreementwas obtainedwiththe

experi-mental values. However,

it

was observed that the NOE’s

showedvery

little

dependenceon andthatinterglycosidic

NOE’s had maxima near conformers

Gl+

and G3+. For

conformer

Gl+,

H3a interglycosidicNOE’sare bigger than

those

of

H3e, whilefor conformerG3+ the reserve is true. Hence,aslightincreaseinthe populationofwellWG1+,would leadtogoodagreement betweentheaveragedNOE’sand the experimental data. The occupancyofwellWG3+mustremain low,ortherelative magnitudeoftheH3a-H3eNOE’s would change.

A

relativeenergy between wellsWG1+,WG2+,and WG3+ of 1.2:0:3 kcal/mol, equivalent to a population of

13:86:1, was found togive the best

fit.

Only the ratio for

WG1+andWG2+was altered, theone for WG2+andWG3+ being kept fixed as that found from the potential energy

calculations. The

( , )

ensemble averaged NOE’s were

calculatedforthe threestaggered 9 rotamersandexhibited

no majordependencyon 9, except thoseinvolvingH9(Table

III).

Sinceother rotamersfor 8 can bepresent,

( , )

ensemble averagedNOEcalculationswere alsodonefor allstaggered 8 rotamers. Forthe g"rotamer,energy wellssimilar tothose fortheg+rotamerwere observed, andagood

fit

ofall NOE’s, exceptfor

H8-H6,

couldbeobtained (Table

III).

Distinct

wells WG1-, WG2-, and WG3“ could be defined by the 6

kcal/mollevelwithrespecttoconformerG2" (Figure2B). The relativeenergyofwellWG1"hadtobemodifiedfora good

figure 7: ID NOEdifference spectraof

aNeuAc(2-8)aNeuAc(2-8)/3NeuAc(c-b-a)for saturationofH3aofresidueaandc(a),of

H3eofresiduec,andofH8 andH9ofresidueb(c)are shown along

withthe ID spectrum(d).

fit.

The relative energy

of

well WG3" was not altered. Relative energiesforwellsWG1",WG2“,andWG3™of0.5:0:2

kcal/molequivalent toa populationof8:90:2 gavethe best agreement between the averagedNOE’sandtheexperimental data. Poor agreementwas foundforthe transrotamer (Figure 2C),sinceno energeticallyfavored conformersnear = -50°

were present where stronginterglycosidic NOE’swiththetwo

H3 geminalresonances occurred.

Trisaccharide.

NMR

experimentswere performedon the trisaccharide in order to compare the linkage conformation

ofthe polymer to theoneofthe linkagec-bofthetrisaccharide

aNeuAc(2-8) aNeuAc(2-8)0NeuAc,(c-b-a). The

ID

NOE

spectra for the trisaccharide at 600 MHz and 288 K are

plotted inFigure7,and theNOEdataare givenin Table V. Byperforming the experimentsat alower temperature, the correlation time

of

the molecule was decreased, leading to bigger negative NOE’s, which couldbemore accurately

in-tegrated. The chemicalshiftassignments andcoupling

con-stants were similartothosereported before (Michonet al., 1987).

Asfor colominicacid,astrongNOEbetween¿>H8andZ>H6,

(8)

Biochemistry,

the 7 = 60° and 8 = 60° rotamerswere predominant in

solution. Due topartialoverlapof6H9and6H8resonances,

the6H9resonance could notbeselectivelysaturatedand the

smallNOEbetween H9 andH7, which might indicate the presence of other 8 rotamers, could not be evaluated, as observed forcolominic acid.

Four sets of NOE’s could be used to evaluate the

( , )

linkage conformation distribution, namely interglycosidic

NOE’s between cH3a-6H8, cH3e-6H8,

cH3a-iH6,

and

cH3e-6H6. AlthoughthecH3a-6H7andcH3e-6H7 NOE’s couldbe observed,the overlapofthe 6H7resonance withthe

6H5resonance preventedtheir quantification. The¿>H8-cH5

NOEwas detected, but its magnitude

(<1)

and the noisy baseline prevented its accurate determination.

All

NOEcalculationswere done usingthe coordinates

of

the disaccharideo¡NeuAc(2-8)aNeuAc, whichcorrespondto residuesc-b ofthetrisaccharide (TableV). TheNOE

con-straintsmapswere similar totheones for colominicacid, and they did not showthepresenceofapreferred conformer in

solution (data notshown). However, the

( , )

ensemble

av-eragedNOE’s,usingmodifiedenergy surfacesforthe gauche rotamers of 8, were able to reproduce adequately the

ex-perimental NOE’s. Relativeenergiesfor WG1+, WG2+, and WG3+ of 0.4:0:3 kcal/mol, equivalent to a population of

20:79:1, were found toincreasethe magnitudeofthe

inter-glycosidicNOE’scomparable tothose

of

the observedones.

The

( , )

ensemble averagedNOEcalculationsfor

g'

andthe transrotamersof 8were performedusing thesame potential

energy surfaces asforcolominicacid.

Discussion

The conformation

of

colominic acid has been previously discussed by a number

of

authors, and all have relied on

interpretation

of

NMR

results. Lindonet al. (1984) deter-mined,from

NMR

at 360MHz,thatH7andH8weregauche

andmolecularmechanicscalculationswere usedtoassessthe

rotational barriers about the C7-C8 bond.

All

staggered rotamerswere found tobeaccessiblewithbarriersofabout

10kcal/mol. The13C

NMR

spin-lattice relaxation times,were

interpreted as suggesting that the

a(2-8)NeuAc

poly-saccharidetumbled isotropically in solutionasarigidspecies.

Michonetal.(1987) studied differencesin NOE’sat 500MHz between the polysaccharide and trisaccharide and from a

qualitative interpretationoftheNOE’sonly,

it

was proposed

thatthe polysaccharide adoptedadifferent conformation from the trisaccharide. Recently, Yamasaki and Bacon (1991), fromaquantitativeanalysisof2DNOE’sat 500

MHz

using

rigid conformers, suggested that the polysaccharide adopts orderedhelical structures in solution.

Inour study,boththe results andtheir interpretationdiffer

fromthoseofYamasaki and Bacon (1991). Differentchemical

shiftsforthepolymerwere observed,whichcould possiblybe

attributed to sample preparation. While the H8 and the

downfieldH9resonance overlappedfor theirsample,theywere

resolvedinthis study. Thus, the overlapoftheH8 andH9

resonances prevented theseauthorsfromdetermining theC8 stereochemistry. Usingrigidmodels and steric constraints, they proposed ordered helical structuresforthefollowing

( , )

ranges:

(-60°

to 0°, 115° to 175°) for 8 = 60°and (90°

to 120°, 55° to 175°) for 8 =

-60°.

Their

( , )

ranges correspond to thetwoareasintheNOEmap(Figure6), where

some NOEconstraints intersect the most. Frommodels,they estimated the numberofturns perhelix,n, tobe from 3 to

4 and the pitch (nh) to be from 9 to 11 Á. Their helical parameters were overestimatedby a factor of2, since it is difficultfrommolecular models alone to determine therotation

angle(µ) along thehelixaxis betweentworesidues,from which

=

2 /µ.

Valuesofngreater than2for 8 = 60° and also

ngreater than2for 8 = -60° correspond totheir

( , )

ranges

(Figure 2).

Inthis study,NOEdataat600

MHz

forthe polysaccharide andthe trisaccharidewere interpretedbyinvokingflexibility

about the exocyclic linkages. Thebest

fit

oftheNOEdata

forcolominic acid (Table

III,

Figure 5)was obtainedfrom

a

( , )

ensemble average over the whole energy surface. Proton couplingconstants andNOEdataindicatedthatthe

g+ rotamers for o>7 and 8 were predominant in solution.

However,flexibilityhad tobeinvoked about theC7-C8bond due toNOE’s which could onlyarisefrom other rotamers, most probably the g"one. From the determination of the proton couplingconstantsfortheH9resonances,allstaggered conformersforthehydroxymethylgroup at C9werepostulated

tobe accessible. Hence, dueto the widerange

of

conforma-tionswhichcan besampled,the polysaccharideissuggested

to exist predominantly as a random coilin solution. As Perez andVergelati (1985)notedintheirstudyof po-lysaccharidehelicalstructures, the spatialorganizationofthe polymerchaincan bedefined by consecutivefragments which

havewell-definedhelicalparameters. Theselocalhelicescan

alsobereferredtoapseudohelices. Compared to other hom-opolysaccharides,a(2-8)-linkedsialicacid ranksfirstinterms

of

displaying awide range

of

helical structures (Figure 2). Obviously, thepresenceoffourbondsinthe linkage junction amplifiesthenumberofallowedconformationalstates,aswell

asthe numberofhelicaltypeswhichcan begenerated. The helicalparametersforafew low-energy conformersare given

inTable

II.

Threehelicesfortheg+rotamers

of

a>7and 8

are shownin Figure8. Wheneverthevalues h = 0 or =

2 are crossed,thechirality ofthehelixchanges. The = 2

helixcorrespondstoazigzagplanarconfiguration, whileh =

0 correspondsto cyclic oligomers. Conformers withsmall values

of

h would foldbackon themselves after nresidues. For the 8 =

g+ rotamer, most energetically favored

con-formerscouldformlocalhelices, since the h= 0linecrosses

a regionwhere values

of

nwere greater than4 (Figure2A).

Also, high-orderhelicescan form with > 6,while forthe other 8 rotamersnisfrom2to3 only. For theg+rotamer

ofo>8inthe high-order helical region,asmall changeinlinkage

conformationleadstoalargechangein helicalparameters. Hence, the topological featuresofthe polymercanchangewith

little

changein energy. Suchproperties wouldbefavorable to topological rearrangements fromdisordered randomcoils tomore orderedconformations which promotetheformation

ofthehelicalepitope.

Forapolysaccharide,theNOE’s

will

beaveragedover all

the conformerssampledin solution.

If

a predominant

con-formeror apseudohelix existsin highenoughproportion, this

shouldbereflectedintheNOE’s,andaNOEconstraints map

could detectthe presence

of

apreferred conformer.

If

more

thanone conformer satisfied the constraints,or nopreferred

conformerwas found, then thepresenceofmolecularflexibility mustbeinvokedto explainthe observedNOE’s. Even

if

the NOE’s indicatethepresenceofapreferredconformerandthe motionalaveragingcalculationsstillsatisfytheexperimental conditions, motional

flexibility

cannot beruled out.

For thecase ofcolominic acidandthe trisaccharide, the

NOE’sare bestexplained by motional averaging. A small proportionofconformerswas found togreatly influence the averaged NOE’s, since their NOE’swere ofmuch greater

magnitude than themajority

of

conformers,as can beseen

(9)

con-Conformation ofMeningococcalB Polysaccharide Biochemistry, Vol. 31,No. 21, 1992 5003

figure 8: Side and top viewwithrespect to thehelixaxisforhelicesofa(2-8)NeuAc10 which

G2+, and G3+. The linkage conformationhavebeenslightlyaltered to giveintegralhelicesofr

for poly(A)isshownon top. Thecharged groupsinthe moleculesare representedas spheres.

formersGl+and G2+ (Tables

III

andV). Therelativeenergy

of

the potential energy wells had to be altered in order to reproducethe observedNOE’s. Empiricalpotentials, which neglect molecularflexibility,electronic interactions, and solvent effect, are used only tocrudely estimatetheallowable

con-formationalspace. Therigid potential wouldalsooverestimate barrierstointerconversion. TheNOEdatacan thusbeused

totestdifferent population distributions calculatedfrom

em-pirical potentialenergy functions(Gumming

&

Carver, 1987). For colominic acid a relative population between wells WG1+ and WG2+ of 15:100 was found to reproduce the NOE’s correctly. Forthetrisaccharide,a ratioof25:100for

thesame wellswas needed. Therelative population

of

well WG3+ to well WG2+ must remainlow(1-2%) in bothcases

or theHe3-H8wouldbecomelarger thantheH3a-H8 NOE.

Hence, differenceinlinkage conformation between thepolymer andshort oligosaccharidescan beexplainedasarisingfrom

slightchangesintherelative populationdistributionof

con-formersinsolution,asopposedto different rigidconformations

(Michonet al., 1987).

Theabovemodelfortheconformational behaviorof

colo-minicacid in solutionhasimportant biological implications. The cross-reactivityofIgMNOVwithboth thea(2-8)NeuAc

polymerand poly(A)can now berationalized(Kabatet al., 1988), sincethey bothcan adoptsimilarhelices (Figure2). From the crystal structure of trinucleoside diphosphate of

adenosine,amodelforthepoly(A) helixwas proposedwith

= 9andh = 2.82

Á

(Saenger et al., 1975). Energetically preferredconformers due tofavorablebasestackingcan form

helicesfrom = 8to12(Yathindra &Sundaralingam, 1976).

Therefore, helicesforthea(2-8)NeuAcpolymerandpoly(A)

can easilybegeneratedwhichhavesimilar helicalparameters. The = 9helixforboth polymersisshowin Figure8. There

isnot onlya similarityin the spatialdistributionofcharges betweenthecarboxylgroupsof a(2-8)-linkedsialicacid and the phosphate groupof poly(A) butalsoastrikingresemblance

betweenthehelical parameters ofboth polymers (Figure2).

Thisobservationwouldtendtosuggestthattheconformational

epitopeoccurs withinone turn

of

thehelix

of

a(2-8)-linked

sialic acidorpoly(A). Sincethe energetically preferred helices

of poly(A) have more than 8 residues perhelicalturn,

it

is

proposedthattheconformationalepitopeforthe<x(2-8)NeuAc

polymerprobablyoccurs withinahigh-order helix which has an extendedconformation (Figure8). However, there isso

farno indicationoftheexactnumberofresidueswithinthis helix that actually bind to group B polysaccharide specific antibodies.

Theunusuallength requirementof a(2-8)-linkedsialicacid oligosaccharides to bind to group B meningococcal poly-saccharidespecific antibodiescan alsoberationalized. Jen-nings et al. (1985) and Finne andMakela(1985)observedthat at leastadecasaccharidewas neededtoinhibitor bind tothese

antibodies. Also,forlarge oligomers

of

up to 17sialic acid

residues,theinhibitorypropertiesdidnotmaximizebutsteadily

progressedwithincreasingsize. Hayrinenetal.(1989) showed

thatthecriticalchain lengthforbindingwas 10units which contributed90%ofthebindingenergy. Thebinding forlonger oligomersalsosteadily progressedwithincreasingsizebutwith minor contributions tothebindingenergyfromtheadditional

residues. Becauseofthelimitationsofthesizeofan antibody

site(maximum6 or 7residues) (Kabat, 1960), these

obser-vations donot imply thattheantibodywas bindingtoasmany as 10 or more consecutive residues, rather that at least 10

residuesare requiredforthe recognitionsite toform.

If

the conformationalepitope corresponds toahigh-order helix with an extendedhelical conformation, as suggested from

cross-reactivityofIgMNOVtopoly(A),large oligosaccharideswould

be required in order for the epitope to form. Since poly-saccharides haveto undergotopologicalrearrangementsfrom disordered randomcoils tomore ordered conformations fa-vorable to theformation

of

thehelical epitopeand because

(10)

Biochemistry,

unlikely that the epitope would occur in any short

oligo-saccharidesequence. Inadditionforthe decasaccharide, the

conformational behaviors

of

the reducingandnonreducing residuesare expected tobedifferent from that ofthe inner residues,asobservedforthetrisaccharideandcolominicacid (Michonet al., 1987). Thecontinued increasein bindingabove 10units couldbeattributed tothelength stabilizationofthe epitope, i.e.,theincreasedprobability

of

the presenceofthe epitope.

The poorimmunogenicityofthe groupBpolysaccharide probably arises from the recognition ofa helical structure

whichisalsoanintegralcomponentoftheneural cell adhesion molecule

N-CAM

(Finneet al., 1983). Despitestructural

mimicry withmammaliantissue,antibodies specificforthe

a(2-8)-linkedsialic acid homopolymercan beproducedand fromthe examples wherebindingstudies havebeenreported

(Jennings et al., 1985; Finne

&

Makela, 1985;Hayrinen et· al., 1989;Kabatet al., 1988) allare specificforthe extended helicalepitope. Becauseour conformationalstudiesindicate thatthis epitopeisonlyaminor contributorto thetotalnumber

of epitopes available, we must therefore presume that the dominanceofthis epitopeintheimmuneresponsemustbethe resultofimmunologicalselection. Thefailureoftheimmune systemtoproduceantibodies specificforthemore populous

lowerorder helices presentin thepolysacchariderandomcoil probably occurs because these shorthelices are

conforma-tionallysimilarto theonesfound in shorter sialyloligomers.

Theseshorta(2-8)NeuAcoligosaccharidesare also present

in humantissue(Finneet al., 1983), andthe production of

specificantibodytothem appears tobeeven more stringently

avoided.

Acknowledgments

We thank FrancisMichonforcriticalreview ofthe

man-uscriptandRobertPonforhelp insamplepreparations. We

are grateful to Andy Byrd and

Bill

Eagan for access to a

preliminarymanuscripton NOE analysis. References

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Figure

Table I: MM2-Minimized Coordinates of aNeuAc-O-Me
figure 1: Structure of aNeuAc(2-8)aNeuAc showing the four torsion angles which determine the linkage conformation with  (06-C6-C7-07) =  7 = 60° and (07-C7-C8-Q8) =  8 = 60°
figure 3: Partial NMR spectra of colominic acid at 600 MHz and 343 K: (a) spin simulated spectrum and (b) resolution enhanced spectrum.
Table IV: Distances for aNeuAc Obtained from Minimized Coordinates, from Distance Extrapolation0 of Calculated 2D NOE Using Conformer Gl+, and from the Experimental 2D NOE6 buildup Rate for Colominic Acid
+3

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