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Cholesteric liquid crystalline phases given by three helical biological polymers : DNA, PBLG and xanthan.
A comparative analysis of their textures
F. Livolant
To cite this version:
F. Livolant. Cholesteric liquid crystalline phases given by three helical biological polymers : DNA, PBLG and xanthan. A comparative analysis of their textures. Journal de Physique, 1986, 47 (9), pp.1605-1616. �10.1051/jphys:019860047090160500�. �jpa-00210359�
Cholesteric liquid crystalline phases given by three helical biological polymers : DNA, PBLG and xanthan.
A comparative analysis of their
texturesF. Livolant
Centre de Biologie Cellulaire (CNRS et EPHE),
67, rue Maurice Günsbourg, 94200 Ivry-sur-Seine, France
(Reçu le 26 novembre 1985, accepté sous forme définitive le 13 mai 1986)
Résumé. 2014 Des phases cristallines liquides cholestériques ont été obtenues avec trois polymères d’intérêt biolo- gique : un polypeptide (le PBLG), un polynucléotide (l’ADN) et un polysaccharide (le xanthane). Les défauts et textures des phases obtenues avec ces trois molécules sont analysés et comparés. La différence essentielle concerne
les coniques focales qui sont absentes dans le PBLG, rares dans l’ADN et très fréquentes dans le xanthane. Un dénombrement des dislocations de rotation et de translation, tenant compte des orientations moléculaires dans le
coeur des défauts, montre que les disinclinaisons - 03C0 sont exclusivement de type 03BB-, les disinclinaisons + 03C0 le
plus souvent de type 03BB+. Des différences apparaissent entre polymères dans la répartition des dislocations de translation mais dans les trois cas les défauts correspondant à l’addition d’une seule couche peuvent être des deux types possibles (03C4- 03BB+ ou 03BB- 03C4+), ce qui différencie ces polymères des petites molécules étudiées jusqu’a présent.
Les principales textures décrites dans les cristaux liquides classiques sont obtenues également avec ces polymères (textures planaires, textures riches en disinclinaisons, textures polygonales). Elles sont cependant plus difficiles à
analyser, au moins dans l’ADN et le xanthane car le pas cholestérique peut être très faible (inférieur au pouvoir
de résolution du microscope).
Abstract 2014 The cholesteric liquid crystalline phases of three polymers of biological interest have been investigated:
PBLG (a polypeptide), DNA (a polynucleotide) and xanthan (a polysaccharide). The textures (and the defects which they contain) of these three mesophases are analysed and compared The main difference concerns focal lines which apparently do not occur in PBLG, are rare in DNA but occur frequently in xanthan. The frequency of
occurrence of the different types of rotation and translation dislocations were measured : - 03C0 disclinations are
always of the 03BB- type and + 03C0 disclinations are mainly 03BB+. Among polymers, differences exist in the distribution of translation dislocations but in these three cases, when only one layer is added, the defect may be either 03C4- 03BB+
or 03BB- 03C4+ which distinguishes polymer mesophases from those of small molecules previously studied The main textures found in classical (small molecule) cholesteric phases were also obtained (i.e. planar textures, textures show- ing numerous disclinations and polygonal textures). However, they are more difficult to analyse especially for DNA
and xanthan mesophases where the helicoidal pitches are small and may not be resolvable in an optical microscope.
Classification
Physics Abstracts
61.30 - 61.70
1. Introduction
There are many
examples
ofliquid crystalline poly-
mers. Most are of
biological
interest andbelong
todifferent biochemical groups such as
polypeptides, polysaccharides
andpolynucleotides (nucleic acids).
Among
these,poly-y-benzyl-L-glutamate (PBLG)
has been the most
extensively
studied This is asynthe-
tic
polypeptide
whichgives
cholestericphases
inconcentrated solution in various
organic
solvents(such
as dioxane,methylene
chloride,chloroform) [1-3].
Theliquid crystalline properties
of nucleic acidswere
reported by
Robinson[2]
and Lerman[4]
forDNA
(desoxyribonucleic acid)
andby Spencer
et al.[5]
for r-RNA
(ribonucleic
acid). In recent years, nume-rous
polysaccharides
have been found togive
choles-teric
liquid crystalline phases
in aqueous solution :hydroxypropyl
cellulose[6-10], schizophyllan [11-13], scleroglucan [14]
and xanthan[1 S-17].
Although
thephysicochemical properties
of thesepolymer
solutions have beenextensively
studied, theoptical
textures of thesemesophases
have never beenthoroughly investigated
We decided therefore to carry out thisstudy
and to make a double compara-Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphys:019860047090160500
tive
analysis, firstly
between the differentpolymer
mesophases andsecondly
betweenpolymer
meso-phases
and small-molecule cholestericphases
whosetextures were the only
examples previously
consi-dered
We have chosen three
polymers belonging
todifferent biochemical groups : a
polypeptide (PBLG),
a
polysaccharide (xanthan)
and a nucleic acid(DNA)
and we have
improved
theexperimental techniques
for
obtaining liquid crystalline phases
of each of thesepolymers
in areproducible
way. In aprevious
work, the structure of the cholestericdroplets appearing
inthe
isotropic phase
wasanalyzed
andcompared
withthe structure of
spherulites given by
classicalliquid crystals
such as twisted MBBA or PAA[18].
In thepresent
study
we consider the textures oflarge-
molecule cholesteric
phases.
Differences revealedby
this
comparative
analysis raise new fundamental pro- blems in theunderstanding
ofliquid
crystalline geometry.Moreover,
precise
textureanalyses
of this kind appear to be necessary if we want to understand themorphologies
ofliving
systems made of suchpoly-
mers.
2. Materials and methods.
2.1 MATERIALS. - Calf
thymus
DNA(Merck)
wassolubilized in 15 mM Tris-Cl- buffer, pH 8,
by magnetically stirring
for 24 h. To obtain short DNAfragments
the solution was sonicated with a Branson sonifier B 15 P(20
kHz, 50W),
for timesranging
from 5 to 35 s,
by
successivepulses
of 5 sinterrupted by resting periods
of 15 s. The solution wasalways kept
at 0 OC. Each DNA fraction wasprecipitated
in ethanol, air dried and diluted in 10 mM Tris-Cl- buffer (pH 8) with 1 mM EDTA. These stock solutionswere stored at 4 °C.
In each fraction, the
length
of the DNA moleculeswas estimated
by electrophoresis
on agarosegels by comparison
with DNA ofclearly
definedlength (Lambda
DNA cutby
HindIII). They
are as follow :Three methods were
developed
to obtain cholestericliquid crystalline phases
with sonicated DNA from fractions 4 to 7.(i) According
to the first method,previously
repor- tedby
Lerman[4], ýJ
DNA(Polymer
and SaltInduced
DNA) was obtained
by mixing
DNAwith
a neutralpolymer
in the presence of monovalent salts. Aphase
segragation occurred and DNA concentrated in onephase
andprecipitated
Good results were obtained with a wide range of concentrations. However,usually,
a solution of 400mg/ml
ofpolyethylene glycol
(PEG; MM 8,000,Sigma)
and 2M KCl wasadded drop
by
drop to an equal volume of the DNA solution (1mg/ml
in 10 mM Tris-Cl- buffer, pH 8).This
mixing
took about 30 min under continuousmagnetic stirring.
DNAprecipitates
weredeposited
between slide and
coverslip
and a cholesteric orga- nizationappeared
in a few minutes at theperiphery.
(ii)
In the second method, adrop
of 10mg/ml
DNA was
slowly
mixed with anequal
volume of a0.4 M KCI solution and
placed
between slide andcoverslip. Preparations
were stored at 4 °C. As the solution became more concentrated thesample
divi-ded into small domains surrounded
by
air. A choles- tericorganization appeared
in theseregions
afterseveral
days
and remained for a few weeks. Thisprocedure
is derived from that of Robinson(1)
but weused KCI instead of NaCI as the monovalent salt
(iii)
Adrop
of ahighly
concentrated DNA solution(50
mg/ml
in 10 mM Tris-Cl- buffer,pH
8) wasdeposited
between slide andcoverslip.
Thepreparation
was
kept
in a humid chamber either at 4 °C or 20 OC.The cholesteric
organization appeared
one or a fewdays
later.’These methods may appear very different. However
only
two conditions areabsolutely
necessary for theproduction
of these cholestericphases : relatively
short chains of DNA (less than 3 pm) and a
high
DNAconcentration.
- Two kinds of
poly-y-benzyl-L-glutamate
wereused : PBLG (MM 28,000,
Sigma)
and PBLG (MM 20,000)synthesized by
the Centre deBiophy- sique
Mol6culaire(Orl6ans, France).
A small amountof
powder
wasplaced
on a slide, adrop
of dioxanadded and
immediately
covered with acoverslip.
- Xanthan is a
polysaccharide
secretedby
thebacteria Xanthomonas campestris. It was
purified
andkindly provided by
Drs. Rinaudo and Milas(CERMAV,
CNRS, Grenoble, France). Thispolymer (MM ,200,000) gives
cholestericphases
in aqueoussolutions
(distilled
water, 60%
NaCI or KCIsolutions).
Preparations
were made aspreviously
described with PBLG.These three
polymers
are all helicoidal and their chemical formulae aregiven
infigure
1 :The
hydrated
form of DNA(B
formDNA)
is aright-handed
double helicoidal molecule whose dia- meterequals
2 nm and helicalpitch
3.4 nm. The twostrands are
antiparallel
and coiled around each other.They
are linkedtogether by hydrogen
bonds which form between the bases of eachpair [10].
PBLG exists as an a helix in the cholesteric
phase.
The
cylindrical
molecule is about 1.8 nm in diameter.Two successive residues which are
projected
ontothe helical axis repeat at intervals of
approximately
0.15 nm [20].
Fig. 1. - Chemical formulae of the three biological polymers
used in this study.
The structure of xanthan has been the
subject
ofconsiderable debate. It would be a fivefold
right-
handed helix whose
pitch equals
4.7 nm with side-chains
packed along
thepolymer
backbone[21,22].
2.2 MICROSCOPICAL TECHNIQUES. - All prepara- tions were studied with a Leitz
(Orthoplan Pol)
or aNikon
(Optiphot
XPol) polarizing microscope,
eitherbetween crossed
polars
or between circularpolarizers
of
opposite
sense. To determine the molecular orien-tations, a quartz first order retardation
plate
wasinserted at 450 between
polarizer
andanalyser.
Theuse of
circularly polarized light
is very convenientsince under these conditions it is not necessary to orientate the
layers
at 450 for thebanding
to be seenand the whole of a
fingerprint
pattern is therefore apparent at the same time.In a cholesteric structure, the molecular orientation
rotates
continuously,
each orientationrecoming
aftera 1800 rotation. This
organization
isrepresented
infigure
2 with the helicoidal axisparallel
to theplane
of the
drawing.
In this situation, when the cholesteric axis is oriented at 450 between crossedpolars,
theintensity
of transmittedlight depends
on the molecular orientation and follows a sine curve. Theintensity
ismaximum when molecules lie in the
plane
of thepreparation
and minimum whenthey
areparallel
to the
microscope
axis(Fig
2b,c).
The cholestericorganization
is revealedby
an alternation ofbright
and dark bands and the
period corresponds
to thehalf-helicoidal
pitch.
Thispitch
can be measureddirectly
inregions
where the helicoidal axis isexactly
horizontal;larger
values would be obtained inregions
where the cholesteric axis is
slightly oblique.
2.3 DRAWING CONVENTIONS. -
According
to thenail convention, molecules are
represented by
lines,nails and dots when
they
arerespectively parallel,
Fig. 2. - Optical properties of the cholesteric organization.
According to the nail convention molecules are represented by lines, nails and points when they are respectively parallel, oblique or normal to the observation plane. When the helical axis of a cholesteric structure is in the plane of the prepara-
tion, molecules are alternatively parallel, oblique and nor-
mal to the observation plane (a). When this structure is
oriented at 450 between crossed polars (P, A), the intensity
of transmitted light depends on the molecular orientation and follows a sinusoidal curve. The intensity is maximum
when molecules are in the plane of the preparation and mini-
mum when they are parallel to the microscope axis (b). The
cholesteric organization is visualized by an alternation of
bright and dark bands (c), the distance separating two bands being the half-helical pitch pl2.
oblique
and normal to theplane
of thedrawing.
Thehead of the nail indicates the
extremity
of the molecule which ispointed
towards the observer. In several cases, nails have been omitted toclarify
thedrawing.
3. Results.
The
general
appearance of theliquid crystalline phases
differ
significantly
from onepolymer
to the other.In
particular
the half-helicoidalpitch (p/2)
can be aslarge
as 1 J.1m in DNA, 20 lim in xanthan and 100 g in PBLG. The smallest valuesofp/2
cannot be resolvedby
thelight microscope. They
can reach 0.1 to 0.2 gm in DNA and xanthan and these twopolymers
thereforereflect
circularly polarized light
in the visible range.The other differences are described below in the
analysis
of defect lines and textures.3.1 DEFECT LINES. - Defect lines are of three types : disclinations, dislocations and focal lines. It often
happens
that certain lines are absent : forexample
focal lines which were never observed in PBLG, are
rare in DNA but are
frequent
in xanthan. The different types of defects encountered with eachpolymer
areshown in table I and their relative
frequencies
intable II and III.
Defect lines
(disclinations
andedge-dislocations)
may be studied more readily in two main situations,
which
correspond
to the two main orientations of the cholesteric axis, eitherparallel
or normal to the pre- parationplane.
Thepath
of the defect line can beeasily
followed in the second case and this kind of
analysis
has been used for
liquid crystals by
Friedel[23],
Cano [24] and
Bouligand [25].
Such lines were also followed in the differentpolymers. They
areanalysed
and
compared
to those found in small-moleculeliquid crystals
in another paper(Livolant,
inpreparation).
However, in
polymers,
this orientation does not allowa
precise analysis
of molecular orientations in thecore of the defects. Therefore, in this
study
we haveinvestigated
the alternative orientation, where thedefect line is normal to the
preparation plane.
Disclinations can be
regarded
as eithertriple points corresponding
to thejunction
of threelayers
(-n)
or as
layers
whichabruptly disappear
( + a). In eachcase, the core of the defect may be continuous or discontinuous
depending
on whether the molecules lieparallel (A)
or normal(r)
to the defect line. These situations and their occurrence are summarized in table II.In the three materials, - n disclinations
always
appear as a black core between crossed polars
(linear
or
circular)
and are therefore of the A- type. + n disclinations occur in all threepolymers
but the £+Table I. - Different types of defects encountered in
DNA, PBLG and xanthan.
Table II. - Relative
.frequencies
of disclinations observed in DNA, PBLG and xanthan.type is much more
frequent
thant the T + type(which
isonly rarely
encountered in DNA andxanthan).
T + disclinations were never observed in PBLG.
In the two commonest situations, A- and
A+,
molecules lie
parallel
to the defect linealong
its coreand there is no
discontinuity
in the molecular orien- tations. K16man and Friedel[19]
noted that this situation was the mostlikely.
Table III. - Counting
of all
dislocations observed in well-resolved cholesteric regions of DNA, PBLG and xanthan.For each value of the
Burgers’
vector(from p/2
to4 p)
the twopossible
situations in the core of the defect were differentiatedTwo disclinations
(one positive
and onenegative)
may be associated to form either
elementary pinches
oredge-dislocations.
We shall consideronly
theedge-
dislocations in thisstudy.
Translation dislocations are numerous in these
phases
but it is often difficult to ascertain whetherthey
are pure
edge-dislocations,
pure screw-dislocations or acombination of both. Each dislocation
corresponds
to the addition or removal of one or more
layers
in thesystem. A
histogram
of thelength
of the observedBurgers’
vector isgiven
infigure
3, for eachpolymer.
These counts were made in selected areas where the cholesteric stratification could be
easily
followedIn DNA and xanthan, dislocations
corresponding
tothe addition of one
layers (pl2)
areprevalent,
repre-senting respectively
57 and 85%
of the total, the other types of dislocationbecoming increasingly
rare as thelength
of the Burgers’ vector increases. On the otherhand, in PBLG, the
length
of Burgers’ vectorsis p
ingeneral (or
amultiple of p)
andonly
11%
of dislo-cations have
half-integral
values.We can also
distinguish
the twopossible
situationsin the core of the defect for each value of the
Burgers’
vector. These data are collected in table III and are
represented by
different conventionalsigns
in thehistogram
offigure
3.When one
layer only
is .added(corresponding
to aBurgers’
vector oflength p/2),
the twopossible
situa-tions T - Å. + and A - T ’ both occur in each of the three
polymers.
However, the first(T - A’)
is favoured(62
%
in DNA, 55%
in PBLG and 77%
inxanthan).
It has been shown
previously
that in MBBAdoped
with a chiral
twisting
agent, this situation was syste-maticaly adopted
[25, 26].When two
layers
are added(b
=p),
the situation Å. - Å. + is theonly
one observed in PBLG and xanthan.It is
predominant
in DNA and the alternative situation(T - T ’)
representsonly 5 %.
For the
highest
values of b, except in DNA where threelayers
areoccasionally
added(b
= 3p/2
and thedefect is of the type T-
Å. +),
wealways
observe the addition of an even number oflayers (b
= 2 p, 3 p, 4 p and so on) and the A- Å. + situation is theonly
oneobserved.
Fig. 3. - Histogram of the length of the observed Burgers’
vectors associated to the edge-dislocations which are
encountered in the three polymers.
3.2 TExTum. - Three types of cholesteric textures are defined in terms of the type of defects which
they
contain :
-
planar
textures with dislocationsonly;
-
polygonal
textures with dislocations and focalconics ;
- fan textures with dislocations, disclinations and focal conics.
3.2.1 Planar textures. - The conditions
required
to obtain
planar
cholesteric textures vary frompolymer
topolymer, presumably
due to thediffering anchoring
conditions of molecules to theglass
sur-faces. Planar textures are
quite easily
obtained withDNA
in 0
conditions with very thinpreparations
and with xanthan when the
polymer
is diluted in distilled water instead of a saline solution.Planar cholesteric structures have a strong rotatory
power, and reflect
circularly polarized light
WithDNA and xanthan, we obtained this reflection in the visible spectrum. This
optical
effect is very strong in xanthan where a spectrum can be seen as alarge
bandparallel
to theedge
of thecoverslip.
Localizedregions
with either smaller and
larger pitches
lie on eithersides of the band. Such series of
parallel stripes,
withrainbow colours, were sometimes obtained in DNA cholesteric
preparations
when the solution penetrates into aclevage
in a KCIcrystal.
These colours do notdepend
on the orientation of thepolars
and are nottherefore
birefringence
colours. We verified thatthey
are due to a reflection of
circularly polarized light
since
they
can beextinguished by
a quater-waveplate
À/4 followedby
a polar in conditions which aredetailed below.
The
wavelength (£o)
of reflected and transmittedcircularly polarized lights
isproportional
to thehelicoidal
pitch
of the structure. For smallpitches,
aBragg
reflection occurs and the relationAo
= pnapplies
when the incidentlight
is normal to the strati- fication(p being
the helicoidalpitch
and n the average refraction index of the structure)[2].
The reflected colours reveal that in DNA and xanthan the helicoidalpitch
may reach valuesranging
from 0.2 to 0.4 J.1m if n is taken as about 1.5. Such colours were neverobtained with PBLG.
The handedness of the cholesteric structure may be determined
by
theanalysis
of thiscircularly polarized light
Indeed, it is well known that for small helicalpitches,
thelight illuminating
a cholestericstructure is
split
into two components, one transmitted and the other reflected, bothbeing circularly polarized,
but in
opposite
senses. For a left-handed cholesteric structure, the reflectedlight
is leftcircularly polarized
and the transmitted
light
isright circularly polarized
The situation is reversed when the cholesteric
phase
is
right-handed
The nature of transmitted and reflectedlight
may beeasily
determinedby
the use of aÀ./4 plate
followedby
apolar.
The slow axis(ns)
of theÀ./4 plate
isalways
oriented at 450 relative to theanalyser
direction but two situations are possible(Fig.
4a, b). The first orientation ofÀ/4
(a)extinguishes right-handed
circularly polarizedlight
whereas the second one (b)extinguishes
left-handedcircularly polarized light.
In themicroscope,
the coloured spectrum of xanthandisappears
in situation b which indicates that the transmittedlight
iscircularly
pola-rized and left-handed.
Conversely,
with reflectedlight,
colours areextinguished
in situation a. It canthen be deduced that xanthan has a
right-handed
cholesteric
organization.
3.2.2 Textures
showing
numerous disclinations. - There are severalpossible
texturesaccording
to therelative
disposition
of defects. Patterns found in cholestericphases
of small molecules also occur for the threepolymers
studied i.e. thequadrilateral
patterns and thezig-zag
lines first described in MBBAdoped
with cholesterol benzoate
[27].
The quadrilateral patterns (Pi. II c, e)
correspond
to the association of four disclinations
(two - n
andtwo + n).
The zig-zag lines (Pl. II b, d) are due to a
regular
alternation of + 1t and - n disclinations. The black
zig-zag
lines indicate theplaces
where molecules areparallel
to one of the twopolars.
These lines separatetwo domains with two different orientations of the cholesteric axis. In the present case
they
were obtainedin a
glass capillary
filled with thepolymer
solution.Fig. 4. - Two orientations of a quater-wave plate (AI4)
oriented at 45° with respect to the polar A. The arrowed direction corresponds to the slow axis of the plate. Right-
handed circularly polarized light is extinguished in situa-
tion (a) while left-handed polarized light is extinguished in
situation (b). (From Robinson, 1966.)
The
zig-zag
line runsparallel
to theedge
of thecapillary
and separates the
peripheral
part of thepreparation
in which
layers
arealigned parallel
to theglass
surfaceand the inner part in which
layers
are rotatedby
900.Regions showing numerous double spirals (Pl. II
g
may be of different kinds :
(i)
It can be aphase
formedby
fusion of cholestericspherulites
since cholestericglobules frequently
showa double
spiral
pattern [28, 29].Plate I. - Table summerizing disclinations and dislocations presented by DNA, PBLG and xanthan. The different defects
are schematically drawn and illustrated Observations between crossed polars.
- n disclinations may be eitherr or A but this latter situation is the only observed with the three polymers.
Edge-dislocations are separated according to the molecular orientations in the core of the defect and to the number of added
layers. The rare situation i - T ’ ( + p) in DNA has to be considered with care but we think that it is really that occurring here.
Plate II. - Textures with numerous disclinations in DNA
(e, t), PBLG (a, b, c) and xanthan (d). Observations between crossed linear polars (a-e) or between crossed circular polars (0.
a : large region showing a population of odd defects ( x 360).
b : region rich in disclinations drawing numerous zig-zag
lines and also a curved dark line because in this region the
helical pitch varies significantly ( x 360).
c : zig-zag lines and quadrilateral patterns near the interface with the isotropic phase ( x 265).
d : zig-zag line running parallel to the side of the glass capillary filled with the polymer solution ( x 360).
e : quadrilateral patterns in a concentrated DNA region
limited by air (x 965).
f : numerous spiralized patterns in DNA ( x 385).
(ii) They
may also beproduced by
distortion of aplanar
cholesteric texture with formation of anticlinal domes andsynclinal
basins. This leads topolygonal
textures in which double
spirals
may be observed in theplane
of focus when the half-helicoidalpitch
is suffi-ciently large.
(iii) Finally,
the cholestericlayers
may besimply
coiled and the
spiral
patternscorrespond
therefore toa transverse view of defects such as the «
tear-drop »
whose structure was
analysed by Bouligand
[25]and presented
again by Bouligand
and Livolant[29].
Regions showing
numerousspirals
have aregular
array of disclinations : + 1t disclinations are localized
Plate III. - Polygonal textures in DNA (b) and xanthan
(a, c, d, e, f, g, h, i). Observations between crossed linear
polars.
a : large region of regular quadratic polygonal fields in
xanthan (NaCI) (x 240).
lb : a small domain with polygons in DNA ( x 320).
c : polygonal fields showing elongated draught-board pat-
terns in xanthan (NaCI) (x 550).
d, e, f : polygonal fields with star patterns observed in xanthan (NaCI). The three micrographs correspond to the
same region : d is focused on the coverslip plane, f on the
slide plane and e in between ( x 325).
g, h, i : distorted polygonal fields obtained with xanthan
(KCl). The same region is focused in the coverslip plane (g),
in the slide plane (i) and in between (h) ( x 480).
at the centre of the
spirals
whereas - n disclinationsare due
mainly
to thepacking
of threespiral
domains.These double spirals are hither left-handed or
right-
handed in PBLG and DNA.
3.2.3
Polygonal
textures. -Polygonal
textures werenever observed with PBLG and
they
areextremely
rare in DNA
(Pl.
IIIb). They
are however veryfrequent
in xanthan and show a
large diversity
of pattern. Someexamples
are shown inplate
III. They were obtainedin various conditions