201
3oumalofhfolecularSh-ucture.113 (1984)201-212 ElsevlerSclencePubhskrs BV, Amsterdam-_~dInTheNetherlands
BIOLOGICAL
APPLICATIONS
PHASE TRANSITIONS
IN
HENRY H.
MANTSCH
Divlslon
of
OF FOURIER
TRANSFORM INFRARED
SPECTROSCOPY.
A STUDY OF
BIOMEHBRANES
Matlonal
Chemistry,
Research
of
CouncJl
Canada.
Ottawa,
KIA
OR6
(Canada)
ABSTRACT The thermal response of aqueous lipid membranes has been investigated by Fourier transform infrared spectroscopy. Changes in infrared spectral parameters are applied to the analysis of the structural changes which occur within the lipid bllayer as the temperature is varied. Such stud1 es prove de the basis for the interpretation of phase transitions in complex bl omembranes.
INTRODUCTION When studying spectroscopy
complex
one
classical
spectroscopist
generally
small
the
of
field
transform The
of
of
UV or
biological
water
a fact
conventional the
impair both
which
advent , along
spectroscopy
has
with
the
has
opened examples
from
our
polymorphism infrared plasma
in
laboratory membranes of
spectroscopy, membrane
0022~2860/34/SO3
of
00
live
to
recent
The
taken
of
by the
of problems
in
Fourier
answers.
solvent
a range
of
require of
widely an aqueous
choice,
measurements
heavy
water
or
severely
the
study
interferometrlc
blol
systems.
and
precluded
hand11 ng techniques, ogl cal
kinds
particularly
invarlantly
the
onal
encountered
structure
many
and
useful
spectroscopic water
spectroscopy of
are
encompasses
only
vi brat1
that
molecular
infrared
almost
of
but
often
part
itself.
not
infrared
However,
not
the
provide
which
use from
there
which
can
is
structure does
of
appl lcatlons
water
Raman techniques,
absorbers,
to
structures
whereby
molecular
the
While
details
science
by the
different
Nevertheless,
spectroscopy
molecular
environment,
quite
solving
biological
domain
samples
a situation
molecules.
infrared
different
bl ologlcal
faces
Fourier
which
ln
Ottawa
to
the
and
I shall range
characterization,
temperature-induced
using strong
limited of
aqueous
of for
the
to the
bacteria.
0 1984 Glsevler Science E’ubh_sbers B V.
ESR,
of
systems. infrared
study
data of
aqueous
of
llpld
illustrate study
by Fourier changes
KMR,
appl lcation
sophisticated
use from
the Infrared
the
transform
availability
up new avenues
are
in
the
this
are
transform structure
of
the
EXPERIHENTAL Instrmentatr
ferr
on
field
The
of
infrared
llcludlng
sophisticated
llplds
and
hereon
were
transform
aqueous
low
with
instruments and
to refs.
1 and
Spectra
aqJisition
various
this
no:
and
models
lipids
conventional
below,
changes
at
in
and
band
above
experiments
are bath
selected
a spectrum,
This
been
response
to
in
live
covered
in
absorption
subtract
the
modern
should
the
masks
several
namely and
as that
determined Among the
of
greatly
routinely various
deconvolutlon
extremely useful
(whereby for
sample
changes
modern
in in
study
IS
Frequency
lineshape of
band
is
often
are
take
into
required
operation main
to for
precautions
recorded
they
with
cells
recorded
at
of
the
account
the
bandwidth than
task
of
values
+ 0.05
technique
removed
contours
to
spectrum.
better the
twc
digitized
and
of
methods,
to
water
range
As the
IS
a routine
are
that
order
the
uncertalntles
a known
spectra and
temperature
it
however.
spectrometers
reduction
rhe
water
of
simplified. 71th
data
the
spectra.
temperature
from deterioration.
bands IS
nhicn
alternative
preparations.
lipid
process
computer
recording
the
bacteria
lipid
6,7),
materials
the
live
Spectra increments
This
Ar
a wide
subtraction
window
spectral
allows
all
(refs.
that
3.4).
study
as
temperature
of
the
Absorbance
for
In it
in
study.
while
the
such
temperature
continuously
since
solvent
spectrometers
(refs.
at
transitIons
mount.
spectrometer
waits
spectrum
5)
and
under
the
temperature,
preventing
water
of
of
system
apparatus cell
range
same
temperature.
on auxiliary
sample
useful
the
bands.
output is
of
well
behavior
the phase
of
a thermostated the
IS of
temperature-induced
and
temperature
(ref.
corresponding
dependent
minutes
D,D)
water
same temperature
Since
studies
Fourier
are
of
a function
control
another
bacteria
fnfrared
the
particularly
pathlength
processing
last
discussed
of
phase
spectrum
as
particular
the
the
be considered,
identical
the
under
records
a few or
infrared
all
to
increase found
Water (H,C
advantages
thermotroplc
the
temperatures,
lncrerents
then IS
has
many
completely
equlllbratlon.
be
at
according
brought
approach
for
results
instruments
infrared
parameter-s
circulating
recorded
the
the
temperature
records
dispersive
studying
collecting
temperature
be
suitable
the
available
handling
Variable
being
quite
experimental The
in
now widely
here, tne interested reader is referred
variable
can
are
instrumentation.
towards
involve
temperatures
usually
which All
be discussed
data
directed
monitoring
are
dramatlcally are
2.
Experiments memb,-ane
cost
changed
spectrometers
preparations.
osler
shall
has
infrared
membrane
obtained
documented
and
lnstrumentatlon
Fourier-transfor;n
years.
of
cm-1
band
from
the
comprised
of
data
now can (ref.
be 8).
narrowing
or
spectra),
IS
more
one
than
a
203 component
; the
integrated of
this
LIPID
method
PHASES-
The of
deconvoluted
lntensjtles to
the
primary
book
level
introduction
to
by Ueissmann
are
as in
to
an
hydrophobic interface
yield
a rather
aqueous
of
especially
polar
their
temperatures
are
into groups.
ability direct
IS
to
in
correct
refs.
dl scussl
on
9-11.
the
the
the
take
up a variety
An
be
found
in
the
of
separated
of
the from
in
parts. e
a hydro-
conmfon to
hydrophobic other
properties
of
at of
the
bllayer
sufficiently
each
structures
segregation
of
bonds
A property
characteristic
this
1.
can
same molecule
by chemical
segregation
of
of
embedded
behavior.
Many
an arrangement
12).
proterns (bottom).
in
together
IS Figure
membranes
(ref.
regions,
consequences
the
membranes
blologlcal
independent
distinct
found
as shown in
presence
linked
environment
moieties
of
Claiborne
by the part,
be
but
An appropriate
biological
membrane with lipid membrane
characterized
a hydrophlllc
can
structure
subJect and
bands
retained.
TRANSITIONS
of
a bilayer the
narrower
are bands
organization
into
and
flexible
apolar
of
lipids
edited
Lipids
lipids
overlapped
Model of a biological (top), and typical
Fig. 1. of lipids
phobic
locate
has
rrequencies
STRUCTURE AND STRUCTURAL
amphlphlllc
excellent
spectrum
and
and by lipids
different polar
all
and
an and
With regard to studies of the polymorphism
in membrane lipids, the infrared
spectrum can be separated to great advantage into spectral regions nhlch inate from possible For
to
the
trum
vlbratlons refer
purpose
of
an
of to
of
aqueous
different
molecular
“head-group’
and/or
“hydrocarbon
tnis,
illustrating membrane
In
moleties.
Figure
preparation
tail”
2 shows
obtained
this
from
manner
spectral
a typlcal human
orrgit
IS
regions.
Infrared
spec-
erythrocytes.
t i 2-
.-w.
C-V
WAVENlJMBER,cti’
Infrared spectrum of aqueous dispersions of human erythrocyte phosFIJ. 2. phatidylethanolamine ‘n water (DaO) recorded in a 6um thick BaF, cell with a Digllab FTS-11 Fourier transform spectrometer equipped with a mercury cadmium tellurlde detector (ref. 13).
The
structural
by monitoring Among
the
stretching red
spectra
temperatures. membranes.
changes various
vibrational vibrations of
egg
occurring
infrared modes of
of
the
maJor
acyl
yo 1 k lecithin
Lecl th i ns are
in
aqueous
absorption
the
diagnostic
chal in
bands
ns.
the
most
membranes
as
a function
value
Figure C-H
lIpId
are
the
3 displays
stretching
cwrsnon phosphollplds
can of
be
methylene a series
region In
studled
temperature.
at
C-H of
different
mammalian
infra-
205
3000
2900
2950
WAVENUMBER
Fig, 3. Temperature-induced lecithin in the region of with increasing temperature.
The
vibrations
infrared (refs. and
of
spectra 14-20).
symetric
2872
o-n-l
methyl
are
changes in the C-H stretching
acyl
chains
of
esters
of
The
strong
bands
fatty at
are
readily and
2920
sL.retching
modes.
asymnetric
and
symmetric
bands
exhibit
of
width
these
which
can
be
infrared bands;
acids
the All
and
CM’
CH,
group.
frequency
the
the
2800
2850
and
spectra of egg the peak height
assigned other
2850
are
the
CH,
comparison
methylene-chain cm-l
respectively;
by
the
weaker
stretching
to
antlsynnnetrlc bands
modes
structural
with
compounds
at
of
tenperature-dependent
related
yolk decreases
2955
the
and
temmlnal
variations
changes
at
the
in
molecular
1 eve1 . Illustrated frequency stearoyl lstlc
in of
those
C16:O
in
frequency
calorimetric and
The highly
whereas
found
band
lecithin.
tne
dlsordered
s.1 gmo~ da1
4 are cm-l
conformationally
hydrocarbons,
ing
Figure 292G
(Cl8:O) of
ationally as
the
54OC for
acyl llquld
the
in
values
above with
can
transition, C18:O
values
ordered
lecithin
acyl 2923 a high The
be taken 1-e.
24°C (ref.
profiles
(C14:0),
frequency
chains
Tm,
temperature
myristoyl
hydrocarbons.
curve, phase
detailed
below
chains m-1
are
midpoint
for 21).
the
2920 as
content
as
obtained
palmitoyl
the
cm-l
found
are
in
characteristic of
gauche
of
the
midpoint C14:0,
for
(C16:O)
the and
character-
solid-like of
confom-
conformers
such
steep of
the
41.5”C
correspondfor
the
10
20
3.0
40
50
60
TEMPEPATURE
Fig. 4. Temperature-dependence stretching bands In the sp ectra and stearoyl lecithin (squares). computing the centre of gravity (for details see ref. 83.
There
IS
stretching
and In
such
effect The
in
the
gel
and
spllttlng
due
helm of
the
eratures chains
only
rocking
In
CH,
an
acyl
scissoring
between behave
like
chain and
from
at in
At
1470
and
of
CH,
trans/gauche the
at
higher
the
similar
to
Tm IS
for
modes
at
chain
independently
Cl6:O
structure
720
show modes
phase
temperatures packing of
and
subcell
IS each
of
above
field
17,
26-29).
has
been
at
temperatures
Tp. where (ref.
and CH,
interchaIn
hexagonal other
chains Tp the
[refs.
50°C
bllayers
correlation
change
lack
at
the
acyl below
an-l
by
and of
saturated
orthorhombic-like
rccklng
rotors
35°C the
vlbratlonal
characterized
acyl
the
conformational
frequency
temperatures
a solid-solid an
of
average
frequency
with
Tp.
packing
Tp and Tm the rigid
is
Cl4:0,
lecithins
at
of
the
this
in
a change
coupling
leclthlns
as a transition
Tp to
in
modes
lnterchaln
pretransition
characterized
of
degree
monitor
higher
frequencies
n-alkanes.
14OC for
temperature
“prerransltlon”,
CH, to
3 (at
of
the
on the to
increase
melting
observed
as the
used the
steep
that
depend
been
22-25);
the
Figure the
phase,
to
scissoring
The
In
literature
chains
The
at
90
the frequency of tne antlsynnnetrlc CH, myrlstoyl (triangles), palmitoyl (circles) Infrared frequencies were obtained by wide seqment of the bands of the topmost 2 an-l
have
(rafs.
disorder.
80
of of
the
acyl
and
systems
indicate
referred
in
long can
observed
arrows
ClS:O),
of
hence
conformatlonal the
evidence
bands
disorder ratio
ample
73
’ C
coupling At
tempindividual
29).
for
207 Figure of
5 shows
temperature
cl
in
10
the
change
the
spectra
30
20
JO
in
the
of
50
60
TEtPESA-uRE
There
IS
a large
the
lipid
phase
observed acyl chain the
with
Tm and The
length
and
greater
The the
at
chal ns.
the
temperature
amounts
change
in
bandwidth.
incubation
proteins
of by
the
In
the
gel
chain
GII-l
band
and
stearoyl
as
a function lecithin.
phase the
at
the
the
or
occurs.
(ref.
32-34).
packing
has
relative
(ref.
annealed The
at
effects
through The changed
22,
30,
this
another
infrared resulting
of
with
at
Tm),
affects llpld
CH1
31). near
4°C
a
transformation
phase
spectra In
the
the
acyl
increasing
temperatures of
in
membranes
bandwidth
of
bandwith
introduced
leclthln
0
clearly
nature
increasing
Tm decreases
protein
the Cl6
in
introduced
disorder
and
the change
with
into
of
but
correlate
disorder
greater
at
a smaller,
to
Tm increases
frequency
are
Tm and
the
cholesterol
temperature
at 3/4 peak height of C14:O (triangles),
dlfflcult
to
at
frequency
membranes
increasing
acyl
both
cholesterol
subtransition
the
of
width spectra
values,
AHm (i.e.
or
change
lecithin
IS
related
the
The
It
bandwldth
greater
of
2920
53
bandwidth
bandwidth
in
incorporated
reversed
the
Uhlle
directly
dependence
transformat?on
as
IS
60
70
the
When hydrated
known
Tp
change
modes.
of
in
Tp.
absolute
incorporation
stretchlng
be
at
the
palmitoyl
of the full bands in the (squares).
increase
increase
of
‘C
Fig. 5. Temperature-dependence antisytnnetric CH2 stretching (circles) and C18.0 1ecTthlns
identifiable
width
myristoyl,
can
transition, show that
a more
rlgldly
after
208 packed
gel
reduced; in
phase
this
hydration.
Thus
dehydration In
and
certain
obtalned
1 ine
phase been
as
that
the
that
the
of
indicated
established
cr
from
converts
by
head
X-r*y
and
contain
to
macroscopic
freeze
fracture
1s greatly are
in
respectively
acyl
typlcal
a ml ccl
structure
It
has
been
concentration of
the
phase
shown
of
transition
gauche
amine
further to
the
in
frequency
of
such
F gure the
gel
shift phase
force
in
the
acyl
this
(ref.
frequency
phase
of
the
a frequency crystal
of
about
1 cm-l Both
CH,
gauche
for
egg
shl ft
of
about
50°C
transitions
transition
the
formation
Since
population mode
yolk
wth
reversible.
this of
is
the
an
phosphatidyl
2 an-l (A
associated are
Induced
18).
stretching
plot
ohase
at
the
solld-like (part C). hexagonal
increasing
triggers 13,
has
36).
thermally 1s the
which
ln
The
llqu’d
5).
this
(refs.
Increase
to
(C to
chains
temperatures
a traasltlon.
7 shows
behind
rearrangement,
the
higher
a further
phase,
rrith
miceliar
at
involves
monitor
driving structural
bonds
phase
llquld-crystallIne
associateo
the
a major
non-bllayer
adequate ethanol
that
requiring
liquid.
non-lamellar
of
techr;iques
chains)
lamellar
lar
Fig. 6. Illustration of the lamellar bllayer structures as ln the gel phase (part A) and ln the liquid-like liquid-crystalline phase Fart 8 shws the non-bilayer structure referred to as the Inverted phase Lonsistrng of tubular inverted mlcelles.
transition
changes
23,35).
unsaturated the
heating
group
result (ref.
erythrocytes,
The
head
transformation
group
(which
further
Fl gure 6.
in
the
the
subtransition
lipid
human
upon
of
causing
and
the
membranes
egg yolk
shell
forces
lncubarlon
hydratlan
phase
hydration
the
phosphollpld
from
crystal
and
suggests
to
at C)
the
18°C and
a
transition
209
.
-
2852
. I -
2851
. I
I. -_v VW 2850.
0
I
_v Tm
10
20
30
40
TEMPERATURE,
The
complexity to
due
provides
to
of
an
which
The
of
In
grown
shows on
a
studies
involving
precludes such
circumventing
8 which
was
spectrum as
fatty
bands. these
monitor
In
acid
bands
acyl the
diet
the
cases
these the
the
the
A frequency
8 contains the
the
use
problems
infrared
addition
observation of
containing
of
deuterium
of of
specifl
oeuterated
(refs.
spectrum
the
frequencies of
trans-gauche
2090
cm-1
of
a hlgl,ly the
of
of
for
upper
of
bands
c 1 lplds
37-41). whole
This
IS
membranes
of
labelled
ordered llmlt
cm-l,
fatty
the
membrane.
in
gel being
the CD,
phase about
lipid
of
cm-l,
are
chain, CH,
acyl
(refs.
a low gauche
2096
the
chains
be used
band
of
Interfering acyl
to
can
ensemble
stretching with
from
bands hence
and bands
a lipld
Similar
CD2 stretching
syrinnetrlc
free as
and
llplds
stretching
a region
incorporated
disorder
ratjo the
from
C-D
IS
the
conformatlonal
average
frequencies,
2200
acid
probe
of
characterisltic
near
fatty
a specific
degree
a variety
temperature-dependent
occur
chains deuterated
provide modes,
on
Figure However
well.
Since
stretching depend
Higher
of
.
proteins the
Figure
and
generally
vibrations.
means
rn
membranes
membranes
well-known
a useful
organism
natural
lipid
exemplified
acids
centre of llpld
BIOMEMBRANES
substances bands
60
Temperature-dependence of the frequency (measured as of the symmetric CH, stretching bands in the spectra obtained from egg yolk phosphatidylethanolamlne.
Fig. 7. gravity) membranes
NATURAL
50
“C
to 5,
42,
43).
IS population. indicative
of
an
increased
populat>on
frequency
and
of
a simple
gel
and
4c
a
of
gauche
conformational
two-component
liquid
crystal
However,
rotamers.
disorder
is
overlapping phases
not
band
(ref.
the
linear.
model
relation
This
to
between
necessitates
obtain
the
the
use
proportions
of
41).
1000
2000
3000 WAVEMJh~BER,cm-l
Fig. 8. laldlan:i
iT-IR spectrum of the bacterial El grown at 30°C in the presence
Figure
9 shows
in
the
spectra
of
live
cells
transition the
gel
The
to phase
isolated
live
are
in
liquid
with
the to
an
between
at
CD,
symmetric
20 and
34OC they
On cooling
stretching
Be1 ow 20°C,
membranes.
a gel
widths
of
bacteria,
the
Thus,
crystalline in
the
phase.
undergo
the
live
aisorder IS
also
4OC higher.
membranes
conformational
phase;
of
Isolated
Acholeplasma acid.
undergo
the
band
membranes a
system
reverts
to
hysteresis.
while
and
liquid
and
crystalline
50 percent
content,
gel
membranes
about
30-C,
blologicai
the
profiles
cells
a slight
membranes
compared
of
temperature
the
However,
temperature
phase
the
tne
isolated
transition.
1 .e.
of
plasma membrane of of perdeuteromyrlstic
the
a given in
important
at
phase live
tl-e
which
bilayer, in
membrane
phase
are the
the
forme-
temperature
is
only
membranes.
lipid
factor
crystal
of
growth
content
cell
liquid
transitions
transition
temperature, the
to
the
about
The IS I.e.,
of
dependent the
for
occurs the
liquid
at
bacteria,
20 percent,
“fluidity”
regulation.
same
as
of on the
amount
crystalline
a
Temperature dependence of the frequency of rhe symmetric CD, Fig. 9. stretching band of the lipids of Acholeplasma laidlaw B grown at 30°C on perdeuteromyr7stIc acid. Shown are frequencies from spectra of live cells with the temperature ascending from 20 to 40°C (+) and descending from 40 to 15°C (x)
and
frequencies
ascendjng
from
5 to
from
spectra
45OC
(a).
of
isolated
membranes
with
the
temperature
REFERENCES 1. 2.
43: 5. 6. 7.
P.R. Grifflths, Chemical Infrared Fourier Transform Spectroscopy, Wlle:J and Sons, New York, 1975, 340 pp. J.R. Ferraro and L.J. Basile (Eds.), Fourier-Transforn Infrared Spectroscopy, Vol s. 1-3, Academic Press, New York, 1982. 0-G. Cameron and R.N. Jones, Applied Spectrosc., 35 (1981) 448. 0-G. Cameron and G.M. Charette. Applied Spectrosc., 35, (1981) 224-225. O.G. Caneron, A. Martin and H.H. Mantsch, Science, 219. (1983) 180-182. D.G. Cameron. H.L. Casal dnd H.H. tlantsch. J. Blochem. Bioohvs._ Methods. 1 (1979) 21-36. 0. Chap-nan. J.C. Gomez-Fernandez, F.M. Goii7 and M. Barnard, J. Blochem. Bioohvs.
8. 9. 10.
Methods
2
(1980)
315-323.
0.G; Cameron, J.K. Kauppinen, Spectrosc., 36 (1982) 245-250. J.K. Kaupplnen, D.J. Hoffatt, 35 (1981 ) 271-276. Spectrosc., J.K. Kaupplnen. 0-J. Moffatt, Optics, 20 (1981) 1866-1879.
D.J.
Moffatt
and
H.H.
Mantsch,
App lied
H-H.
Mantsch
and
D.G.
Cameron,
App lled
0-G.
Cameron
and
H.H.
Mantsch,
App 17ed
212 11.
12. 13. 14. 15. 16. 17. 18. 19. 20. 21_ 22. 23. 24. 25. 26. 27. 28. 29. 30. 31. 32.
Z: 35. 36.
37. 38. 39. 40. 41. 42. 43.
J.K. Kauppinen. D.J. Moffatt, H.H. Mantsch and D.G. Came’on. Analytical Chemistry. 53 (1981) 1454-1457. G. Welssmann and R. Claiborne (Eds.), Cell Membranes, HP Publishing Co., YEW York, 1975, 283 pp. H.H. M-antsch, A. Martin and D.G. Cameron. Can. J. Spectroscopy, 25 (1981) 79-84. R.G. Snyder, S.L. Hsu and S. Krimn, Spectrochlm. Acta, 34A (1978) 395406. D.F.H. Wallach, S.P. Verma and J. Fookson, Blochlm. Biophys. Acta. 559 (1979) 153-208. U.P. Fringe11 and Hs.H. Gtinthard, in E. Grell (Ed.), Membrane Spectroscopy, Springer. Berlin, 1987, pp. 270-332. D.G. Cameron, H.L. Casal and H.H. Mantsch Biochemistry, 19 (1980) 36653672. H.H. Hantsch, A. Hartln and D.G. Cameron, Biochemistry, 20 (1981) 313831 45. H.H. Mantsch, D.G. Cameron, P.A. Tremblay and M. Kates, Bloch?m. Blophys. Acta. 689 (1982) 63-72. H.H.-Mantsch, Sic. Hsl, K.W. Butler and D.G. Cameron, Blochim. Biophys. Acte, 728 (1983) 325-330. D-AUllkinson and J-F. Nagle. Biochemistry, 20 (1981) 187-192. R. Mendelsohn, R. Dluhy, J. Taraschi, D.G. Cameron and H.H. Hantsch, Blochemlstry, 20 (1981) 6699-6’06. D.G. Cameron and H.H. Hantsch, Blophyslcal J., 38 (1982) 175-184. C. Huang, J.R. Lapides and 1-W. Levln, J. Am. Chem. Sot., 104 (1982) 59265930. H.H. Mantsch, A. Garg and D.G. Cameron, Spectroscopy Int. J., 2 (1983) 8896. H.J. Janlak, D.M. Small and G.G. Shipley, Blochemlstry 15 (1976) 45754580. D.G. Cameron, H.L. Casal , E.F. Gudgln and H.H. Mantsch, Biochlm. Blophys. Acta, 596, (1980) 463-467. D.G. Cameron, E.F. Gudgin and H.H. Mantsch, Biochemistry, 20 (1981) 44964500. H.L. Casal, H.H. Hantsch. D.G. Cameron and R.G. Snyder, J. Chem. Phys., 77 (1 S82) 2825-2830. J. Umemura, D-G. Cameron and H.H. Mantsch, Blochlm. Blophys. Acta, 602 (1980) 33-44. M. CortiJo and 0. Chapman, FEBS Lett., 131 (1891) 245-248. S.C. Chen, J.M. Sturtevant and B.J. Gaffney, Proc. Nat. Acad. Sci. US, 77 (1980) 5060-5063. H.H. FUldner, Biochemistry, 20 (1981) 5707-5710. M.J. Ruocco and G.G. Shipley. Blochlm. Blophys. Acta. 684 (1982) 59-66. H.L. Casal . H.H. Mantsch, D.G. Cameron and B.P. Gaber, Chem. Phys. Lipids, 33 (1983) 109-112. R.P. Cullis and B. de Kruiff. Blochim. Blophys. Acta, 559 (1979) 399-420. I.C.P. Smith and H.H. Hantsch, Trends Blochem. Sciences, 4 (1979) 152154. H.L. Casal, I.C.P. Smith, D.G. Cameron and H.H. Mantsch, Blochim. Blophys. Acta, 550 (1979) 145-149. H.L. Casal, D.G. Cameron, I.C.P. Smith and H.H. Mantsch, Biochemistry, 19, (1980) 444-451. H.L. Casal , D.G. Cameron, H.C. Jarrell , 1.C.o. Smith and H.H. Mantsch, Chem. Phys. Llpids, 30 (1982) 17-26. R.A. 3iJhy, R. Mendelsohn, H.L. Casal and H.H. Mantsch, Biochemistry. 22 (1983) 1170-1177. 5. Sunder, D.G. Cameron, H.H. Hantsch and H.J. Bernstein, Can. J. Chern.. 56 (1978) 2121-2126. D.G. Cameron, H.L. Casal, H.H. Hantsch, Y. Boulanger and I.C.P. Smith Biophyslcal J., 35 (1981) 1-16.