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HAL Id: jpa-00210359

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Submitted on 1 Jan 1986

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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�

(2)

Cholesteric liquid crystalline phases given by three helical biological polymers : DNA, PBLG and xanthan.

A comparative analysis of their

textures

F. 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

of

liquid crystalline poly-

mers. Most are of

biological

interest and

belong

to

different biochemical groups such as

polypeptides, polysaccharides

and

polynucleotides (nucleic acids).

Among

these,

poly-y-benzyl-L-glutamate (PBLG)

has been the most

extensively

studied This is a

synthe-

tic

polypeptide

which

gives

cholesteric

phases

in

concentrated solution in various

organic

solvents

(such

as dioxane,

methylene

chloride,

chloroform) [1-3].

The

liquid crystalline properties

of nucleic acids

were

reported by

Robinson

[2]

and Lerman

[4]

for

DNA

(desoxyribonucleic acid)

and

by Spencer

et al.

[5]

for r-RNA

(ribonucleic

acid). In recent years, nume-

rous

polysaccharides

have been found to

give

choles-

teric

liquid crystalline phases

in aqueous solution :

hydroxypropyl

cellulose

[6-10], schizophyllan [11-13], scleroglucan [14]

and xanthan

[1 S-17].

Although

the

physicochemical properties

of these

polymer

solutions have been

extensively

studied, the

optical

textures of these

mesophases

have never been

thoroughly investigated

We decided therefore to carry out this

study

and to make a double compara-

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphys:019860047090160500

(3)

tive

analysis, firstly

between the different

polymer

mesophases and

secondly

between

polymer

meso-

phases

and small-molecule cholesteric

phases

whose

textures were the only

examples previously

consi-

dered

We have chosen three

polymers belonging

to

different biochemical groups : a

polypeptide (PBLG),

a

polysaccharide (xanthan)

and a nucleic acid

(DNA)

and we have

improved

the

experimental techniques

for

obtaining liquid crystalline phases

of each of these

polymers

in a

reproducible

way. In a

previous

work, the structure of the cholesteric

droplets appearing

in

the

isotropic phase

was

analyzed

and

compared

with

the structure of

spherulites given by

classical

liquid crystals

such as twisted MBBA or PAA

[18].

In the

present

study

we consider the textures of

large-

molecule cholesteric

phases.

Differences revealed

by

this

comparative

analysis raise new fundamental pro- blems in the

understanding

of

liquid

crystalline geometry.

Moreover,

precise

texture

analyses

of this kind appear to be necessary if we want to understand the

morphologies

of

living

systems made of such

poly-

mers.

2. Materials and methods.

2.1 MATERIALS. - Calf

thymus

DNA

(Merck)

was

solubilized in 15 mM Tris-Cl- buffer, pH 8,

by magnetically stirring

for 24 h. To obtain short DNA

fragments

the solution was sonicated with a Branson sonifier B 15 P

(20

kHz, 50

W),

for times

ranging

from 5 to 35 s,

by

successive

pulses

of 5 s

interrupted by resting periods

of 15 s. The solution was

always kept

at 0 OC. Each DNA fraction was

precipitated

in ethanol, air dried and diluted in 10 mM Tris-Cl- buffer (pH 8) with 1 mM EDTA. These stock solutions

were stored at 4 °C.

In each fraction, the

length

of the DNA molecules

was estimated

by electrophoresis

on agarose

gels by comparison

with DNA of

clearly

defined

length (Lambda

DNA cut

by

Hind

III). They

are as follow :

Three methods were

developed

to obtain cholesteric

liquid crystalline phases

with sonicated DNA from fractions 4 to 7.

(i) According

to the first method,

previously

repor- ted

by

Lerman

[4], ýJ

DNA

(Polymer

and Salt

Induced

DNA) was obtained

by mixing

DNA

with

a neutral

polymer

in the presence of monovalent salts. A

phase

segragation occurred and DNA concentrated in one

phase

and

precipitated

Good results were obtained with a wide range of concentrations. However,

usually,

a solution of 400

mg/ml

of

polyethylene glycol

(PEG; MM 8,000,

Sigma)

and 2M KCl was

added drop

by

drop to an equal volume of the DNA solution (1

mg/ml

in 10 mM Tris-Cl- buffer, pH 8).

This

mixing

took about 30 min under continuous

magnetic stirring.

DNA

precipitates

were

deposited

between slide and

coverslip

and a cholesteric orga- nization

appeared

in a few minutes at the

periphery.

(ii)

In the second method, a

drop

of 10

mg/ml

DNA was

slowly

mixed with an

equal

volume of a

0.4 M KCI solution and

placed

between slide and

coverslip. Preparations

were stored at 4 °C. As the solution became more concentrated the

sample

divi-

ded into small domains surrounded

by

air. A choles- teric

organization appeared

in these

regions

after

several

days

and remained for a few weeks. This

procedure

is derived from that of Robinson

(1)

but we

used KCI instead of NaCI as the monovalent salt

(iii)

A

drop

of a

highly

concentrated DNA solution

(50

mg/ml

in 10 mM Tris-Cl- buffer,

pH

8) was

deposited

between slide and

coverslip.

The

preparation

was

kept

in a humid chamber either at 4 °C or 20 OC.

The cholesteric

organization appeared

one or a few

days

later.

’These methods may appear very different. However

only

two conditions are

absolutely

necessary for the

production

of these cholesteric

phases : relatively

short chains of DNA (less than 3 pm) and a

high

DNA

concentration.

- Two kinds of

poly-y-benzyl-L-glutamate

were

used : PBLG (MM 28,000,

Sigma)

and PBLG (MM 20,000)

synthesized by

the Centre de

Biophy- sique

Mol6culaire

(Orl6ans, France).

A small amount

of

powder

was

placed

on a slide, a

drop

of dioxan

added and

immediately

covered with a

coverslip.

- Xanthan is a

polysaccharide

secreted

by

the

bacteria Xanthomonas campestris. It was

purified

and

kindly provided by

Drs. Rinaudo and Milas

(CERMAV,

CNRS, Grenoble, France). This

polymer (MM ,200,000) gives

cholesteric

phases

in aqueous

solutions

(distilled

water, 60

%

NaCI or KCI

solutions).

Preparations

were made as

previously

described with PBLG.

These three

polymers

are all helicoidal and their chemical formulae are

given

in

figure

1 :

The

hydrated

form of DNA

(B

form

DNA)

is a

right-handed

double helicoidal molecule whose dia- meter

equals

2 nm and helical

pitch

3.4 nm. The two

strands are

antiparallel

and coiled around each other.

They

are linked

together by hydrogen

bonds which form between the bases of each

pair [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

onto

the helical axis repeat at intervals of

approximately

0.15 nm [20].

(4)

Fig. 1. - Chemical formulae of the three biological polymers

used in this study.

The structure of xanthan has been the

subject

of

considerable debate. It would be a fivefold

right-

handed helix whose

pitch equals

4.7 nm with side-

chains

packed along

the

polymer

backbone

[21,22].

2.2 MICROSCOPICAL TECHNIQUES. - All prepara- tions were studied with a Leitz

(Orthoplan Pol)

or a

Nikon

(Optiphot

X

Pol) polarizing microscope,

either

between crossed

polars

or between circular

polarizers

of

opposite

sense. To determine the molecular orien-

tations, a quartz first order retardation

plate

was

inserted at 450 between

polarizer

and

analyser.

The

use of

circularly polarized light

is very convenient

since under these conditions it is not necessary to orientate the

layers

at 450 for the

banding

to be seen

and the whole of a

fingerprint

pattern is therefore apparent at the same time.

In a cholesteric structure, the molecular orientation

rotates

continuously,

each orientation

recoming

after

a 1800 rotation. This

organization

is

represented

in

figure

2 with the helicoidal axis

parallel

to the

plane

of the

drawing.

In this situation, when the cholesteric axis is oriented at 450 between crossed

polars,

the

intensity

of transmitted

light depends

on the molecular orientation and follows a sine curve. The

intensity

is

maximum when molecules lie in the

plane

of the

preparation

and minimum when

they

are

parallel

to the

microscope

axis

(Fig

2b,

c).

The cholesteric

organization

is revealed

by

an alternation of

bright

and dark bands and the

period corresponds

to the

half-helicoidal

pitch.

This

pitch

can be measured

directly

in

regions

where the helicoidal axis is

exactly

horizontal;

larger

values would be obtained in

regions

where the cholesteric axis is

slightly oblique.

2.3 DRAWING CONVENTIONS. -

According

to the

nail convention, molecules are

represented by

lines,

nails and dots when

they

are

respectively 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 the

plane

of the

drawing.

The

head of the nail indicates the

extremity

of the molecule which is

pointed

towards the observer. In several cases, nails have been omitted to

clarify

the

drawing.

3. Results.

The

general

appearance of the

liquid crystalline phases

differ

significantly

from one

polymer

to the other.

In

particular

the half-helicoidal

pitch (p/2)

can be as

large

as 1 J.1m in DNA, 20 lim in xanthan and 100 g in PBLG. The smallest values

ofp/2

cannot be resolved

by

the

light microscope. They

can reach 0.1 to 0.2 gm in DNA and xanthan and these two

polymers

therefore

reflect

circularly polarized light

in the visible range.

The other differences are described below in the

analysis

of defect lines and textures.

(5)

3.1 DEFECT LINES. - Defect lines are of three types : disclinations, dislocations and focal lines. It often

happens

that certain lines are absent : for

example

focal lines which were never observed in PBLG, are

rare in DNA but are

frequent

in xanthan. The different types of defects encountered with each

polymer

are

shown in table I and their relative

frequencies

in

table II and III.

Defect lines

(disclinations

and

edge-dislocations)

may be studied more readily in two main situations,

which

correspond

to the two main orientations of the cholesteric axis, either

parallel

or normal to the pre- paration

plane.

The

path

of the defect line can be

easily

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 different

polymers. They

are

analysed

and

compared

to those found in small-molecule

liquid crystals

in another paper

(Livolant,

in

preparation).

However, in

polymers,

this orientation does not allow

a

precise analysis

of molecular orientations in the

core of the defects. Therefore, in this

study

we have

investigated

the alternative orientation, where the

defect line is normal to the

preparation plane.

Disclinations can be

regarded

as either

triple points corresponding

to the

junction

of three

layers

(-

n)

or as

layers

which

abruptly disappear

( + a). In each

case, the core of the defect may be continuous or discontinuous

depending

on whether the molecules lie

parallel (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 three

polymers

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

is

only rarely

encountered in DNA and

xanthan).

T + disclinations were never observed in PBLG.

In the two commonest situations, A- and

A+,

molecules lie

parallel

to the defect line

along

its core

and there is no

discontinuity

in the molecular orien- tations. K16man and Friedel

[19]

noted that this situation was the most

likely.

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

to

4 p)

the two

possible

situations in the core of the defect were differentiated

(6)

Two disclinations

(one positive

and one

negative)

may be associated to form either

elementary pinches

or

edge-dislocations.

We shall consider

only

the

edge-

dislocations in this

study.

Translation dislocations are numerous in these

phases

but it is often difficult to ascertain whether

they

are pure

edge-dislocations,

pure screw-dislocations or a

combination of both. Each dislocation

corresponds

to the addition or removal of one or more

layers

in the

system. A

histogram

of the

length

of the observed

Burgers’

vector is

given

in

figure

3, for each

polymer.

These counts were made in selected areas where the cholesteric stratification could be

easily

followed

In DNA and xanthan, dislocations

corresponding

to

the addition of one

layers (pl2)

are

prevalent,

repre-

senting respectively

57 and 85

%

of the total, the other types of dislocation

becoming increasingly

rare as the

length

of the Burgers’ vector increases. On the other

hand, in PBLG, the

length

of Burgers’ vectors

is p

in

general (or

a

multiple of p)

and

only

11

%

of dislo-

cations have

half-integral

values.

We can also

distinguish

the two

possible

situations

in the core of the defect for each value of the

Burgers’

vector. These data are collected in table III and are

represented by

different conventional

signs

in the

histogram

of

figure

3.

When one

layer only

is .added

(corresponding

to a

Burgers’

vector of

length p/2),

the two

possible

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

%

in

xanthan).

It has been shown

previously

that in MBBA

doped

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 the

only

one observed in PBLG and xanthan.

It is

predominant

in DNA and the alternative situation

(T - T ’)

represents

only 5 %.

For the

highest

values of b, except in DNA where three

layers

are

occasionally

added

(b

= 3

p/2

and the

defect is of the type T-

Å. +),

we

always

observe the addition of an even number of

layers (b

= 2 p, 3 p, 4 p and so on) and the A- Å. + situation is the

only

one

observed.

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 dislocations

only;

-

polygonal

textures with dislocations and focal

conics ;

- fan textures with dislocations, disclinations and focal conics.

3.2.1 Planar textures. - The conditions

required

to obtain

planar

cholesteric textures vary from

polymer

to

polymer, presumably

due to the

differing anchoring

conditions of molecules to the

glass

sur-

faces. Planar textures are

quite easily

obtained with

DNA

in 0

conditions with very thin

preparations

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

With

DNA 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 a

large

band

parallel

to the

edge

of the

coverslip.

Localized

regions

with either smaller and

larger pitches

lie on either

sides of the band. Such series of

parallel stripes,

with

rainbow colours, were sometimes obtained in DNA cholesteric

preparations

when the solution penetrates into a

clevage

in a KCI

crystal.

These colours do not

depend

on the orientation of the

polars

and are not

therefore

birefringence

colours. We verified that

they

are due to a reflection of

circularly polarized light

since

they

can be

extinguished by

a quater-wave

plate

À/4 followed

by

a polar in conditions which are

detailed below.

The

wavelength (£o)

of reflected and transmitted

circularly polarized lights

is

proportional

to the

helicoidal

pitch

of the structure. For small

pitches,

a

Bragg

reflection occurs and the relation

Ao

= pn

applies

when the incident

light

is normal to the strati- fication

(p being

the helicoidal

pitch

and n the average refraction index of the structure)

[2].

The reflected colours reveal that in DNA and xanthan the helicoidal

pitch

may reach values

ranging

from 0.2 to 0.4 J.1m if n is taken as about 1.5. Such colours were never

obtained with PBLG.

The handedness of the cholesteric structure may be determined

by

the

analysis

of this

circularly polarized light

Indeed, it is well known that for small helical

pitches,

the

light illuminating

a cholesteric

structure is

split

into two components, one transmitted and the other reflected, both

being circularly polarized,

but in

opposite

senses. For a left-handed cholesteric structure, the reflected

light

is left

circularly polarized

and the transmitted

light

is

right circularly polarized

The situation is reversed when the cholesteric

phase

is

right-handed

The nature of transmitted and reflected

light

may be

easily

determined

by

the use of a

À./4 plate

followed

by

a

polar.

The slow axis

(ns)

of the

À./4 plate

is

always

oriented at 450 relative to the

(7)

analyser

direction but two situations are possible

(Fig.

4a, b). The first orientation of

À/4

(a)

extinguishes right-handed

circularly polarized

light

whereas the second one (b)

extinguishes

left-handed

circularly polarized light.

In the

microscope,

the coloured spectrum of xanthan

disappears

in situation b which indicates that the transmitted

light

is

circularly

pola-

rized and left-handed.

Conversely,

with reflected

light,

colours are

extinguished

in situation a. It can

then be deduced that xanthan has a

right-handed

cholesteric

organization.

3.2.2 Textures

showing

numerous disclinations. - There are several

possible

textures

according

to the

relative

disposition

of defects. Patterns found in cholesteric

phases

of small molecules also occur for the three

polymers

studied i.e. the

quadrilateral

patterns and the

zig-zag

lines first described in MBBA

doped

with cholesterol benzoate

[27].

The quadrilateral patterns (Pi. II c, e)

correspond

to the association of four disclinations

(two - n

and

two + 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 the

places

where molecules are

parallel

to one of the two

polars.

These lines separate

two domains with two different orientations of the cholesteric axis. In the present case

they

were obtained

in a

glass capillary

filled with the

polymer

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 runs

parallel

to the

edge

of the

capillary

and separates the

peripheral

part of the

preparation

in which

layers

are

aligned parallel

to the

glass

surface

and the inner part in which

layers

are rotated

by

900.

Regions showing numerous double spirals (Pl. II

g

may be of different kinds :

(i)

It can be a

phase

formed

by

fusion of cholesteric

spherulites

since cholesteric

globules frequently

show

a 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.

(8)

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 be

produced by

distortion of a

planar

cholesteric texture with formation of anticlinal domes and

synclinal

basins. This leads to

polygonal

textures in which double

spirals

may be observed in the

plane

of focus when the half-helicoidal

pitch

is suffi-

ciently large.

(iii) Finally,

the cholesteric

layers

may be

simply

coiled and the

spiral

patterns

correspond

therefore to

a 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

numerous

spirals

have a

regular

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 disclinations

are due

mainly

to the

packing

of three

spiral

domains.

These double spirals are hither left-handed or

right-

handed in PBLG and DNA.

3.2.3

Polygonal

textures. -

Polygonal

textures were

never observed with PBLG and

they

are

extremely

rare in DNA

(Pl.

III

b). They

are however very

frequent

in xanthan and show a

large diversity

of pattern. Some

examples

are shown in

plate

III. They were obtained

in various conditions

(distilled

water, NaCI or KCI

solutions).

The

polygons

are often square

(from

3 to

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