NOTES ON THE STRUCTURE OF SHELL
AND MEMBRANES OF THE HEN’S EGG;
A STUDY WITH THE SCANNING ELECTRON MICROSCOPE
P.-C.-M. SIMONS G. WIERTZ
Central Institute for Poultry Research « Het Spelderholt n, Beekbergen,
The Netherlands (Director : Ir. P. 1JBBELS)
Laboratory of animal Physiology, Agricultural University, Wageningen,
The Netherlands (Direetor : Prof. A. M. FRENS)
INTRODUCTION
For more than 100 years
microscopic
studies have been made of the structure of the avianegg-shell.
In the eggenvelop
differentlayers
can be discerned termedclassically :
inner and outermembrane, mammillary
and spongylayer
and cuticle.In more recent work we meet with the terms : inner and outer
membrane,
cone andpalisade layer,
surfacecrystal layer
and true cuticle(Ty!,!R, rg6 5 ).
During transport
andhandling
of eggs more than 10 p. 100 may crack. This results in a veryimportant
economic loss. Not very much is known about the struc- tural factors in the shell that have an influence on the resistance of the egg to brea-kage.
More research on shell structure may therefore be useful. Our work(SrMO:!s
and
W WR T Z , zg65 ; E L -B OU S HY ,
SIMONS andWIE R T Z, 19 68)
in which we used thelight microscope
and studies with the aid of the electronmicroscope (S IMONS
andW
I E R T Z
, 19 6 3 , 19 66, 19 68)
may be seen as a contribution in this field. Efforts to exa- mine the surface of fracturesthrough
the calcifiedpart
of the shellby replication technique
were notcompletely
successful because of difficulties inremoving
thereplicas
untorn fromlarger
areas of the fracture surface. So we were veryglad
toget
theopportunity, though only
for one and a halfdays,
to do some research witha
scanning
electronmicroscope.
Without muchpreliminary preparation
the surfacestructure of rather
bulky specimens
can be studied over a wide range ofmagnification
with a
large depth
of focus and ahigh
resolution( 200 A
for the averagespecimens ;
that is about 20times as
good
as the resolutionprovided by
anoptical microscope).
A focussed electron beam strikes the surface of the
object
in i ooo lines. Thepri-
mary electrons of this beam
bring
about the emission ofsecondary
electronsby
theobject.
Thesesecondary
electronstogether
with a few backscatteredprimary
elec-trons are received in a collector that contains an
accelerating electrode,
ascintillator,
a
light pipe
and aphotomultiplier
tube. Theimage
is built up on a cathode ray screen,the
scanning
beam of which issyncronously coupled
to thescanning primary
electronbeam. Because of their
raster-character, photographs
of the cathode rayimage
cannotbe
magnified
many times. As at the contours of any relief in theobject
fewer secon-dary
electrons aretrapped,
these contours show in theimage bright edges (figs.
2,2
8, 2 g).
The egg shell is not a conductor. So it must be coveredby
a thinlayer
ofconducting
material like carbon toprevent
the accumulation ofnegative charges
at its surface.
MATERIAL AND METHODS
Pieces from the waist of egg-shells were glued with Velpon, a cellulose-acetate glue, on to a
round aluminium plate (diameter I cm) and covered with a carbon film by evaporating carbon
in a vacuum chamber. They were examined in the Stereoscan electron microscope of the Institute for Medical Physics in Munster (Western Germany). Pictures were made with a primary voltage
of io kV.
Radial and tangential ground sections were prepared by grinding and polishing one side of
the specimen according to the method of J ONGERIUSand HmN2zsERCEx (1963). However, because of unsatisfactorily polishing, left too many of the grinding scratches, the radial sections had to be discarded. The sections were etched by boiling for Iminutes in a 10p. ioo solution of sodium sulfide.
The technique used for separating the inner from the outer membrane is as follows : saw the cap off the egg at the pointed end. Empty the egg and rinse the interior of the shell several times.
Make a hole at the blunt end through shell and outer membrane. Blow through this hole into the air chamber and the inner membrane will come off.
After soaking the shell for 60minutes in 5 p. 100EDTA at pH 7.2 the true cuticle with most of the pore plaques can be removed from the shell by washing the egg surface with a jet of water.
Part of the calcite of the surface crystal layer will also be removed by this treatment which per- mits a view of the denuded surface of the calcified shell.
RESULTS AND DISCUSSION
( 1 )
I
. True cuticle
The
description by
SIMONS and WWRTZ( 19 66)
of the vesicular structure of the true cuticle withairspaces
between the vesicles could be confirmed. The cuticular surface shows manystar-shaped
cracksystems (fig. z).
Thebig
cracksystems
repre- sent the surfaces of the oval poreplaques
assuggested by
SIMONS and WIFRTZ(ig66).
The diameters of the surfaces of these
plaques
amount to over 100 g. Their surfacesare flatter than the
surrounding
cuticular surface. The smaller cracksystems
elsewhereon the cuticular surface may be caused
by
ashrinking
of the true cuticledirectly
after
oviposition. Looking
into a crack shows cuticular vesicles of up to about I g(fig. 2 ).
S
IMONS and WWRTZ
( 19 66)
mentioned that with the passage of time the cuti- cular surface becomesincreasingly
flatter. The smaller cracksystems
thendisappear gradually possibly
due to athinning
of the true cuticleby
theshrinking
of the vesiclesThe cracks in the pore
plaques
on the other hand increase due to thisshrinkage (fig. 3 ).
( 1
) Un diagramme représentatif de la section radiale de la coquille donne par les auteurs (Plate I) facilite la compr6hension du texte. Note des editeurs.
z. Den.uded
surface of
thecalcified
shellThe denuded surface of the
shell,
visible after removal of the truecuticle,
showspore holes and in some
places
theangular
boundaries of the columns of thepalisade layer
may be seen with diameters of sometimes over 80 !.(figs.
4,g).
So at leastpart
of the surface
crystal layer
hasdisappeared.
The pores are oval with diameters which can amount to more than 40
(figs. 6, 7 ).
Normally
the upperpart
of a pore is filled up with aplug
of cuticular material.Together
with the true cuticle most of theseplugs
were removed.Figure
7 shows a pore in whichpart
of thisplug
is stillpresent.
The wall of the pores is covered with alayer
of
organic
material. Fibrils can be seenrunning parallel
to the surface of the shells(fig. 8)
at a distance of about 2 fLapart. They
may be theedges
of the mattedlayers
of fibrils seen in radial sections
through
thepalisade layer (S IMONS
and WIURTZ,1963, fig. i 3 ),
which have the same relative distance.3
. Shell
fractures
The
scanning
electronmicroscope
is very useful forstudying
fracturesthrough
the shell. It is very
interesting
to see that fractures over thegreater part
of theirlength
runalong
theorganic
matter. Theonly exception
we met with is seen infigure
g(left mammilla)
andfigure
io. This means that thestrength
of theorganic
matter willbe an
important
factor in thebreaking strength
of the shell. This is inagreement
with thepositive
relation between thecompactness
of theorganic
matrix in thepalisade layer
and shellstrength
mentionedby
SIMONSand WIERTZ(zg6 3 ).
The cone
layer composed
of the so-called mammillaepenetrates
the outer mem- brane(figs.
m, 12, i3,i 4 ).
The basal surface of the mammilla is smooth rounded off and covered with a thinlayer
oforganic
material(figs.
9, 11, 12, r3,iq.).
Thislayer
was also seen in radial sections
(S IMONS
andWIE R T Z, 19 6 3 , fig. 10 ).
Just
beneath the base of the mammilla the outer membrane containsirregular
calcified
depositis through
which fibres thatpenetrate
themammillary
base pass in tufts(figs.
m, 12,i 3 ). Except
at thespots
where the fibres enter the mammilla there seems to be no contact between the mammilla and these calcifieddepositions
(figs.
12,13 ). They
have been described earlier(e.
g. SIMONS andWI ERTZ , ig6 3 ;
1EI,-B
OUSHY
,
SIMONS andW I E R T Z , zg68).
The
only
fracturethrough
the calcified centre of a mammilla(figs.
9 to theleft, 10
)
shows the cones, with maximum widths of i5 and 30fL,radiating
from the crys-tallization
centre of the mammilla. At theperiphery
of the cones thecrystallites
seemto be orientated
nearly perpendicular
to the cone surface. At the surface of trans-verse fractures
through
columns(figs. 1 6, 17 )
the same orientation ispresent (Com-
pare the radial
peripheral
striations ofcrystal aggregates
seenby
HEYN,19 6 3 , fig. 6).
The
organic coverings
ofneighbouring mammillary
bases fuse between the mammillae and sometimespenetrate
the shell for more than 70 !.(fig. 11 ).
Fracturesfollow these lines of least resistance
(figs.
m, 12, i3,i 4 ).
At manyplaces
entire conesare broken out of a
mammilla,
the fracturefollowing again
the thinlayer
oforganic
material between the cones
(fig. 11 ). Figures
14 and z5 show that after a iowide
zone,
starting
at the line of contact between two mammillae and rich inorganic
mate-rial,
thequantity
of thisorganic
material between the mammillaedecreases,
the lamella-likecrystallites becoming
visible.Everywhere
in the calcified shell(figs.
15,y , 20 , 22 )
theorganic
matter containsmany
pitlike
holes in whichtiny crystals
can be found(HE YN , rg6 3 ).
Thehighest magnification
we used( X 4 200 )
does notyet permit
a definite conclusion about theirform,
but vague diamond andhexagonal
contoursmight point
to rhombohedra.Figures
4 and 5 of HEYN( 19 6 3 ) give
the sameimpression, though
this author called themirregular.
Thegreatest
diameter of thepitlike
holes infigure
r5 iso.8 and
infigure
17, 0.5 5 g. At thecorresponding
sites in radial sectionsthey
were seen as vesiclesof o. 8 and
o.4diameter (SiMOVS
and WIERTZ,rg6 3 ).
In thepalisade layer
a lar-ger hole was seen
(fig.
20, 3.5[ 1-).
In sections of egg shells from climate-stressed hensE
L -B OUSHY
,
SIMONS and WIERTZ(i 9 68) found
holes with diameters of3 . 1 , 5.8
and 9!.Indeed in
ground
sectionsthrough
these shells muchlarger
cavities werepresent.
In the
palisade layer
theplane
of fractures may deviate from thestrictly
radial direction characteristic of the conelayer.
Here and there transverse breaksthrough
columns of about 50
diameter
arepresent (figs.
m,1 6, 17 )
so that here the fractureruns in a
tangential plane, parallel
to the surface of the shell. But hereagain
thefracture follows thin
layers
oforganic
material(matted
fibrils with attachedvesicles)
which are seen to lie at relative distances of about 2 g
through
the whole of thepali-
sade
layer (S IMONS
and WWRTZ,rg6 3 ).
Thetops
of the rhombiccrystals
visible atthe front side of the broken column in
figure
16give
an indication of several of thesepotential
fractureplanes.
Theselayers
oforganic
material may be seen far moreclearly
infigure
ig at theright
side a little below the middle of thephotograph
andin
figure
2z. The fact that thesetangential layers
of fibrils aremissing
in the conelayer, together
with thegreater
amount oforganic
material between the cones ascompared
with that between thecolumns,
may account for thestrictly
radial courseof the fractures
through
the conelayer.
The surface
crystal layer
isdeposited
ontop
of thepalisade layer (figs.
21,22 ).
It is about 8 fLthick and consists of small calcite
crystals
with theirgreatest
dimen- sion aboutperpendicular
to the egg surface. SIMONS and WIERTZ( 19 6 3 )
observed it in radial sections as a z.5-2wide
zone,predominantly
fibrillar in structure. Inground
sections examined inpolarized light
it varied in thickness between 3 and 8 !,. Thedeposition
of thislayer signifies
the end of the formation of the calcified shell.4
. Ground sections etched with sodium
sulfide
Figures
23 and 24arephotographs
of an etchedtangential ground
sectionthrough
the
palisade layer.
Theirregular
lines oforganic
material between thecrystal
aggre-gates
are visible.Clearly
seen too, aresystems
ofparallel lines, running
in four direc- tions andenclosing rectangles
and diamonds. These formsmight
beexpected
if thegrinding plane
intersects with rhombohedra.Neighbouring aggregates
show linesystems
of different direction. In thepalisade layer crystallites
can be seen of o.7!; i fL(figs.
20,24).
5. Membranes
The inner membrane was
separated
from the outer one andphotographs
weretaken from the
plane
ofseparation
in inward and outward direction(figs.
25,2 6).
The inner membrane is much denser than the outer one. The thickness of the fibres in both membranes
corresponds
with the measurements in sections(S IMONS
andW
WR’
rz, ig6 3 ).
The average fibre diameter in the inner membrane is less than that in the outer membrane. In both membranes fibres often fuse. In the outer membranecomposite
bundles are seen of upto 4 fibres (fig. 2 6).
The4 -fibre
bundle can be followed for more than I mm. There are not many broken fibres at theseparation
surface.The course of the fibres in the membranes shows some orientation. The thicker fibres
run
roughly parallel
insystems forming
diamond meshes. Yet there is some indi-cation of a
predominant direction,
whichmight
account for directional differences instrength
of the membranes within thetangential plane
and for the fact that the membranes may be torn from the shell inspiral strips.
SCHMIDT( 1957 )
found thatthe membrane fibres take a
spiral
course around the egg axis.On the outer surface of the fibres
crystals
may be seen of about o. 5 glength;
at one
place
12crystals
over a distance of8
can be seen.They
may behexagonal
orrhombohedrial in form
(fig. 27 ).
6. Inner
layer of
inner membraneThis flat
layer (fig. 2 8)
hasalready
been describedby
SIMONS and WrEx’rz(rg6 3 ).
In it
granules
with diameter of up to I {1can be seen,lying
in short rows ofroughly
one direction
(figs. 2 8, 2 g).
Thelayer
shows small cracks(probably
causedby
shrink-age),
some of which run in the same direction as the rows ofgranules.
7
. Shell
of
a boiled eggIn a
preliminary
test of theapparatus, pieces
of shell from a boiled egg wereexamined. The
greater part
of the membranes had been removed. The tufts of mem-brane fibres
entering
the mammillae as well as the calcifieddepositions
around thefibres at these
spots
can be seen infigures
30 and 31 which are taken from the inside of the shell. Infigure
30 theedge
of thepiece
of shell lies a little below thetop
ofthe
photograph.
Figure
32depicts
a radial fracturethrough
some mammillae.Interesting
too,are the two rhombohedrial
crystals
of 8 and 16 g diameter attached on theedge
ofa mammilla outside its
organic covering.
The surface of the boiled cuticle is seen in
figure
33. In it many rhombohedrialcrystals
of 2 g diameter arepresent.
TY>~!R( 19 6 4 )
found calcium carbonatecrystals
in the outer cuticular
layer
of Anatidae eggs. HEYN( 19 6 3 )
described small cuticularbumps
fromunderlying crystals.
In hisphotograph
their dimensions are about 0.2 !..We have not
previously
met withcrystals
in the cuticle of hen’s eggs.ACKNOWLEDGEMENTS
The authors thank Prof. Dr. G. PFEFFERKORN and Dr. R. CxRisrErrxuss of the Institute for Medical Physics of Munster University as well as Mr. S. HErrsrxn of the Electron Microscopy Department of Service Institute for Applied Mechanics and Technical Physics at Wageningen
who made this investigation possible. For the reproduction of the photographs thanks are due
to l!Ir. C. VAN EDEN and Mr. C. I. VAN WijK, Wageningen.
SUMMARY
The structure of shell and membranes of the hen’s egg was studied with a Stereoscan electron
microscope. We examined cuticle, denuded surface of the calcified shell, radial fractures, etched
tangential ground sections and membranes. Detailed descriptions and photographs are given.
Fractures show a strictly radial course in the cone layer, but deviations to a tangential plane may
occur locally in the palisa.de layer. In both cases the fracture mostly follows layers of organic
material. The strength of the organic material in the shell may thus be an important factor in
the breaking strength of the egg.
RÉSUMÉ
ÉTUDE DE LA STRUCTURE DE LA COQUILLE ET DES MEMBRANES
COQUILLIÈRES
DE L’œUF DE POULE AU MOYEN DU MICROSCOPE
ÉLECTRONIQUE
STÉRÉOSC.!1BLa structure de la coquille et des membranes coquillières de l’œuf de poule a été étudiée au
microscope électronique Stéréoscan. Nous avons examiné la cuticule, la surface dénudée de la
coquille calcifiée, des fractures radiales, des sections polies tangentielles gravées et les membranes.
Des descriptions détaillées et des photographies sont présentées. Les fractures présentent dans
la couche des cônes un trajet strictement radial mais des déviations vers le plan tangentiel inter-
viennent localement dans la couche en palissade. Dans tous les cas la fracture suit le plus souvent
des couches de matière organique. La solidité de la matière organique de la coquille peut par
conséquent être une composante de la résistance à la rupture de l’oeuf.
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