in vitro evaluation of surfactants with eucalyptus
TRANSCRIPT
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In vitro evaluation of surfactants with eucalyptus oil for
respiratory distress syndrome
R. Banerjee a,b,*, Jayesh R. Bellare c
a School of Medicine, Cardio6ascular Research Institute, Uni6ersity of California, 3333 California Street, Suite 150, San Francisc
CA 94118-1245, USAb School of Biomedical Engineering, Indian Institute of Technology, Bombay, India
c Department of Chemical Engineering, Indian Institute of Technology, Bombay, India
Abstract
The effects of low doses of eucalyptus oil (EO) were studied on the surface properties of phospholipid suspension
as exogenous surfactants, by in vitro analysis using a pulsating bubble surfactometer and a Wilhelmy balanc
Survanta, ALE C and Exosurf, commonly used surfactants in t herapy of respiratory d istress syndrome were used
controls for comparison. The test surfactants, in Ringers lactate at 1%, were pulsated at 40 cpm in the surfactomete
EO caused a significant improvement of adsorption of the surfactants. In the case of the binary mixture
dipalmitoylphosphatidylcholine and phosphatidylethanolamine (2:3), EO significantly improved the adsorptio
stability and minimum surface tension obtained. This combination performed better than ALEC and Exosurf and w
comparable to Survanta with respect to minimum surface tension attained. The re-spreading of a surface excess filof this mixture in a Wilhelmy balance was higher than that of ALEC and Exosurf. The ultrastructure of the E
enriched surfactants using cryogenic scanning electron microscopy showed easy facturability and formation of ope
membranous structures, which could have been associated with the improved surface activity.
Keywords: Mechanics of breathing; Alveolar surfactant; Methods; Wilhelmy balance; Surfactometer; Pharmacological agen
Eucalyptus oil; Surfactant; Phospholipid suspensions; Eucalyptus oil
1. Introduction
Pulmonary surfactant is a complex mixture of avariety of saturated and unsaturated phospho-
lipids, neutral lipids and surfactant specific
proteins SP-A, B, C and D (Wilkinson, 1993)
which lower the surface tension at the airalv
olar interface of the lungs. R espiratory distre
syndrome of neonates is most often due to developmental deficiency of pulmonary surfactan
along with an immature structure of the lun
(Avery, 1959). The predominant phospholipid
lung surfactant is dipalmitoyl phosphatidy
choline. It is capable of achieving near zero su
face tension during monolayer compression bu
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142
cannot function alone as an effective replace-
ment surfactant due to its poor adsorption and
re-spreading. Most surfactants available com-
mercially vary widely in their composition and
biophysical properties. Protein-free surfactants
have a relative disadvantage of poor re-spread-
ing when compared to their natural counter-
parts. The surfactant specific proteins SP-A, Band C are responsible for the rapid adsorption
and re-spreading of natural lung surfactants
(Creuwels et al., 1997). Ho wever, immunogenic
and cost considerations make the search of an
effective and affordable artificial protein-free
surfactant worthwhile in spite of their relative
lower effica cy. I n E xo su rf, t he a dd it io n o f
hexadecanol helps to partially overcome this
disadvantage o f protein-free surfactants by im-
proving the adsorption and re-spreading of the
base phospholipid namely dipalmitoyl phos-phatidylcholine (Yu and Possmayer, 1993). Cer-
t ain o th er n at ur al o ils a nd a lco ho ls co uld
perhaps be used instead of hexadecanol as re-
spreading agents and are the subject of the
present study.
One such natural oil is eucalyptus oil (EO)
which is commonly used as an expectorant in
chronic bronchitis (Gennaro, 1985). The efficacy
of EO in chronic bronchitis was documented by
Siurin (1997) with beneficial effects in a study of
150 patients with chronic bronchitis. Ho wever,
very few studies have described the performance
of this oil as a possible surfactant in respiratory
distress syndrome. Zanker et al. (1980) had eval-
uated the surfactant like effects of commonly
used remedies for colds including EO. They
found a decrease in surface tension at an air
water interface and improved lung compliance
in in vivo animal studies with EO. The present
study evaluates the in vitro performance of EO
as a component of phospholipid based surfac-tants.
The aims of the present study are to compare
the surface properties of different phospholipid
solutions with or without the addition of EO
and to approach the clinical issue of obtaining a
protein-free effective surfactant.
2. Materials and methods
1,2 dipalmitoyl phosphatidylcholine (DPPC
abbreviated here as PC), palmitoyloleoyl pho
phatidylethanolamine (PE) and palmitoyloleo
phosphatidylglycerol (PG) were purchased (a
\99% purity) from the Sigma Chemical C
Calcium chloride was obtained as \98% puri
from Qualigens Fine Chemicals-Glaxo, IndiSterile Ringers lactate solution was obtaine
from Albert David Ltd., India. Exosurf N eon
tal, Survanta and ALEC were obtained as kin
gifts from Burroughs Wellcome Co., Ross Labo
ratories, and Britannia Pharmaceuticals, UK, r
spectively. Technical grade EO, having specifi
gravity 0.91590.005 at 25C, was purchase
from Gopaldas Visram and Co., India. Steri
distilled water and sterile normal saline we
used, as supplied, for reconstitution of Exosu
and ALEC. Other chemicals used in t he experments were HPLC grade chloroform and ac
tone (Qualigens Fine Chemicals-Glaxo, India
Chloroform was used as the spreading solvent.
We studied the effects of EO at low doses (
part oil to 9 parts of phospholipid v/v), on th
surface properties of phospholipid monolaye
by in vitro analysis using a pulsating bubb
surfactometer. This instrument tests the dynam
surface properties of surfactants at a spheric
interface and can be pulsated at high speed
This would be relevant to the lung surfacta
system as pulsation at a high speed of 40 cp
would correspond to the respiratory rate o
neonates (Schubring et al., 1976; Yu and Pos
mayer, 1993) and also to the frequency of vent
lator settings used for neonates (Koyabashi
al., 1990). The minimum surface tension, stat
surface tension at a bubble of maximum size
as a measure of the adsorption to an air liqu
interface, and stability index of liposomal su
pensions of the main phospholipids of pu
monary surfactant and their binary mixed film
in the ratio of 2 parts of PC with 3 parts of Por PG, forming the mixtures PCPE and PCPG
respectively, are studied both in the absence an
in the presence of eucalyptus. The surfactants i
t he p resen ce o f E O a re r efer red t o P CE O
P EE O, P GEO, P CP EE O, a nd P CP GEO. E
was added in the ratio of, 1 part of E
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1
(2 ml) to 9 parts of the phospholipid (single/
mixed). The performance of the test formulations
with EO was compared with that of three differ-
ent commercial surfactants Survanta, ALEC
and Exosurf. This was supplemented by the study
of the performance of E O enriched surfactants on
the re-spreading of phospholipid monolayers us-
ing a Wilhelmy balance. The ultrastructure of
liposomal suspensions of the surfactant formula-
tions with eucalyptus were also studied in an
attempt to analyze the structural changes, if any,
which could explain the effects of EO.
2.1. Pulsating bubble surfactometer experiments
All the test surfactant formulations were stud-
ied in the form of phospholipid suspensions in
Ringers lactate (a polyelectrolyte solution con-
taining 2 mM calcium and buffered to a pH of
7.4). Ringers lactate was used due to its similarity
to the chemical composition of the alveolar fluid
as studied by Nielson (1986). Thin films of 20 ml
of single or mixed phospholipid solution in chlo-
roform (concentration 50 mg/ml) were formed
and the solvent was allowed to evaporate under
nitrogen gas for half an hour. EO was added in
the ratio of, 1 part of EO (2 ml) to 9 parts of the
pho spholipid (single/mixed). The final concentra-
tion of the phospholipid-oil mixture in the liposo-
mal suspension was 1%. The thin film, after
evaporation of the solvent, was dispersed in 100ml of Ringers lactate, shaken by hand and then
left undisturbed at room temperature for 12 h to
allow formation of liposomes by hydration (Yu
and Possmayer, 1993). The therapeutic surfac-
tants were tested after reconstitution in the form
recommended for clinical use in a concentration
of 1 mg phospholipid per ml. Control experiments
were performed using EO suspended in Ringers
lactate in a concentration of 1%.
All samples were tested at 37C in a pulsating
bubble surfactometer (Surfactometer, E lectronet-ics Corp.). This instrument and its use in dynamic
surface pro perty evaluation were first described by
Enhorning (1977). Briefly, a disposable plastic
chamber is loaded with 25 ml of the test sample.
The capillary of t his chamber serves as an airway
for bubble formation. A thermoregulated water
bath surrounds the chamber. The bubble size ca
be changed by manual control from minimum siz
having radius Rmin=400 mm (minimum surfac
a rea Amin=201.1104 mm2) to maximum si
having radius Rmax=550 mm (maximum surfac
area Amax=380.3104 mm2). The bubble can b
pulsated between these two sizes at frequenci
upto 100 cpm. There is a 47% reduction in arewhen the bubble changes size from Rmax
to Rmi
The pressure gradient across the bubble (DP)
measured with the help of a precision transduc
having a pressure range of 010 Torr and sens
tive to very low volume displacements (0.04 ml/c
water). The surface tension at the air liquid inte
face (g) is then calculated at minimum and max
mum bubble size of Rmin and Rmax, respectivel
in accordance with the law of Laplace as applie
to spheres (DPmin=2gmin/Rmin an d DPmax=2gma
Rmax). The bubble was cycled in automatic modbetween Rmin a n d Rmax at 40 cpm for 10 cycle
and the minimum and maximum surface tensio
were measured as surface tension at Rmin an
Rmax, respectively, during pulsation at 40 cpm
Cycling was stopped at Rmin and the bubble wa
expanded manually to Rmax
and held static for 1
sec. The static surface tension was measured. Th
gives an indication of the adsorption of the su
factant at the air liquid interface of the bubble.
correction factor was applied to the static surfac
tension at Rmax by multiplication with the facto0.055/0.040 (equal to the maximum radius/min
mum radius in accordance with Putz et al. (1994
This was done to compensate for t he error arisin
due to the assumption by the inbuilt program o
the pulsating bubble surfactometer of a minimu
radius during start of static measurements b
default. Stability index (SI) was calculated
SI=2(gmaxgmin)/(gmax+gmin) at 40 cp
(Clements et al., 1961). 40 cpm was chosen as th
frequency of oscillation as it corresponds to th
neonatal respiratory rate (Yu and Possmaye1993) and is the frequency which is used clinical
in ventilator settings for a neonate of respirator
distress syndrome (Koyabashi et al., 1990).
Statistical an alysis of the effects of the additiv
wa s d o n e b y t h e M a n n Whitney U test usin
PB0.05 as the cut off level for significance.
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2.2. Wilhelmy balance experiments
Dynamic surface pressure-area (p-A) isotherms
of solvent spread interfacial films were measured
with a Wilhelmy surface balance (LB 5000, KSV
Instruments, Finland). Highly pure triply de-ion-
ized water (Milli-Q UV Plus System, Millipore
Corp.) and acetone were used in all balance clean-
ing procedures. F or subphase formation, sterile
Ringers lactate solution, which contains in mEq/
L N a+ 131, K+ 5, Ca++ 4, bicarbonate as lactate
29 and Cl 111, was used after adjusting to a pH
of 7.4 by adding concentrated NaOH drop-wise.
Surfactants were dissolved in chloroform to a
concentration of 1 mg/ml and the solution was
spread drop-wise from a syringe at the air water
interface under surface excess conditions. This
refers to a high initial surface concentration where
the amount of surfactant spread was greater than
that required for a monolayer coverage (15 A, 2/
molecule). For studying the effect of EO, 1 part of
EO (Gopaldas Visram & Co., In dia) was added t o
9 parts of the chloroform solution of the phos-
pholipid before spreading. All experiments were
carried out at a body temperature of 3790.5C.
A time span of 10 min was allowed for solvent
evaporation before commencing dynamic cycling.
Surface pressure (the difference in the surface
tension of the interface without and with surfac-
tant) was monitored continuously from the force
on a sand-blasted platinum slide. Seven successivecycles of compression/expansion at the interface
were recorded between maximum and minimum
areas of 772.5 and 193.1 cm2 (compression ratio
4:1) at a constant speed of 1.2 cpm. The compres-
sion ratio of 4:1 is much higher than that found in
normal respiratory cycles. However, this ratio was
used in the present study in order to obtain
information regarding the re-spreading capability
of the surfactants. This was done by comparison
of collapse-plateau ratios, which could be ob-
tained only on maximum compression of the filmspast collapse. The speed of 1.2 cpm was the
highest possible by the Wilhelmy balance used.
D ynamic re-spreading was characterized b y col-
lapse plateau ratio criteria of Turcotte et al.
(1977). This parameter cannot be easily judged by
a pulsating bubble surfactometer. Hence, experi-
ments were conducted on a Wilhelmy balance t
study the re-spreading of PCPEEO in compariso
with the commercial surfactants. On a given p-
compression curve, a vertical line is drawn at th
point of steepest slope and a horizontal line
drawn at the post-collapse region. The distan
from the intersection of these lines to the end o
the compression stroke is defined as the collap
plateau length. The re-spreading ratio is given b
the ratio of the lengths of these plateaus for th
seventh and first cycles. A ratio of 1 indicat
complete re-spreading and of 0 indicates no r
spreading. Fig. 1 schematically represents th
method of calculation of this ratio.
2.3. Cryogenic scanning electron microscopy
experiments
All samples were tested as liposomal suspe
sions of 1% concentration as used for the pulsaing bubble surfactometer study. The techniqu
used for sample preparation for cryogenic scan
ning electron microscopy was developed b
Bhadriraju and Bellare (1993). In this cryo-tec
nique, a thin layer of the sample was sandwiche
between two copper meshes that were fixed o
two copper plates. The copper plates used were o
0.1 mm commercial grade copper and the meshe
were squares of:33 mm2. One of the coppe
plates was L-shaped to facilitate fracture of th
sample inside the airlock chamber of the micro
scope. The sandwiched sample was then plunge
rapidly into liquid nitrogen kept at 196C
Samples were kept in liquid nitrogen for 30 mi
and then transferred onto the cryo-stage of th
scanning electron microscope (JEOL 6400 SEM
The samples were then stabilized in the airloc
chamber fracture-stage and then freeze fracture
by removing the L-shaped copper plate with th
microscopes fracture k nife. The fractured samp
together with cryo-stage was then transferred t
the specimen chamber of the microscope. Bo
the fracture-stage in the airlock chamber and thimaging stage in the specimen chamber of th
microscope were maintained at 130C . T h
sample was imaged at an accelerating voltage of
kV and a scanning probe current of 109 A
working distance of 2732 mm and magnific
tions between 1000 and 4000 .
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Fig. 1. Calculation of re-spreading. A schematic representation of isotherms of surface excess films compressed post-collapse in
Wilhelmy balance. The re-spreading ratio is obtained by dividing t he length of the collapse plateau of the seventh cycle to that
first cycle.
Fig. 2. Minimum surface tension on addition of EO. The minimum surface tension on pulsation at 40 cpm in a pulsating bubb
surfactometer is compared for surfactants with and without addition of EO. A lower value of minimum surface tension
physiologically beneficial. All values are means with standard errors with n=5 8.
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Fig. 3. Effect of EO on stability of surfactants. The stability index of the various surfactants in the presence and absence of EO
depicted here. A larger value of the parameter indicates that the film is more stable and capable of maintaining a low tension witho
collapse, for a longer period of time. All values are means with standard errors with n=58.
3. Results
Fig. 2 shows the minimum surface tension at 40
cpm for the test formulations, without and with
EO. The stability indices are compared in Fig. 3
and the values of static surface tension on adsorp-
tion are compared in Fig. 4. EO in buffer, withoutany phospholipids, adsorbed to a surface tension
of 3592 mN /m and on compression reached a
minimum tension of 3091 mN /m.
The attainment of low static surface tension
values indicates the formation of a monolayer film
of the surfactant at the interface and gives a
measure of the adsorption of the compound. The
addition of EO caused a significant improvement
in the adsorption at Rmax of all the surfactant
formulations i.e. caused significant decrease in the
value of static surface tension attained (PB0.05using Mann Whitney U test, n=8). Ho wever,
the addition of EO was detrimental to the stabil-
ity of most surfactants except PG and PCPE.
An improvement in stability and minimum sur-
face tension were also obtained in the case of
PCPEEO. Table 1 summarizes the beneficial ef-
fects of EO on the surface properties of the su
factant formulations.
On comparing the surfactant formulations wi
eucalyptus, and the commercial surfactants, it w
observed that PCPEEO performed particular
well with respect to surface tension reduction wit
significantly lower gmin values when compared tSurvanta. Its adsorption and stability were als
comparable to that of Survanta and it was f
superior to ALEC and Exosurf with respect to a
the parameters considered. We could not test th
r e-sp rea din g o f Su rva nt a d ue t o t ech nic
difficu lt ies in spr ea din g of t he a queou
suspension.
The ability of the surfactants to re-spread to th
air liquid interface on dynamic cycling is also
physiologically important parameter. While com
paring PCPEEO with that of the therapeutic sufactants, only ALEC and Exosurf were used fo
comparison, as we were unable to spread th
aqueous suspension of Survanta as a chloroform
solution at the air liquid interface of the L
t ro ugh . F ig. 5 d ep ict s t he p er fo rm an ce
PCPEEO with respect to minimum surface te
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1
sion, stability index, adsorption and re-spreading
in comparison with ALEC, Exosurf and Sur-
vanta. PCPEEO had a high re-spreading ratio
of 0.7290.03 which was higher than that of
Exosurf and ALEC (0.1890.02 and 0.6590.03,
respectively).
We also compared the ultrastructure of the
surfactants in the absence and presence of euca-
lyptus in a cryogenic scanning electron micro-
scope. The structure of EO alone did not sho
any membrane formation and had a homog
nous stippled appearance of oil micro-drople
in buffer. The surfactants with eucalyptu
formed liposomes, which were easily fracture
to reveal their internal membranous organiz
tion. Wavy membranous folding was more com
monly formed in the case of liposomes co
taining EO.
Fig. 4. Effect of EO addition on adsorption. The static surface tension at Rmax is depicted as a measure of adsorption to t
air liquid interface. A lower value of this parameter indicates more efficient adsorption with more surface-active material reachin
the interface. All values are means with standard errors with n=5 8.
Table 1
Beneficial effects of EO on surface properties-PBS studya
Minimum surface tension (%) Stability index (%) Static surface tension: adsorption at Rmax
(%)Compound
PCEO 22b 50b 37c
PEEO d 37b 14c
33c18cPG EO 43c
PCPEEO 79c 149c 45c
41c 30cPCPG EO 27c
a All comparisons have been made between surfactant in the presence of EO vs surfactant without any additive. The percentag
of change have been calculated.b Indicates a detrimental effect.c Indicates a significant improvement (MannWhitney U test PB0.05).d Indicates absence of any significant change.
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Fig. 5. Comparison of surface properties of PCPEEO and
commercial surfactants. The performance of PCPEEO is com-
pared with that of ALEC, Exosurf and Survanta. The mini-
mum surface tension is measured after pulsation at 40 cpm for
30 sec in a pulsating bubble surfactometer. The static surface
tension is measured at Rmax in a pulsating bubble surfactome-ter as a measure of adsorption. The re-spreading ratio is
measured by comparison of the collapse plateau ratios in
surface excess films in a Wilhelmy balance. No data was
available for the re-spreading of Survanta.
8 mm size, which are fractured revealing the inte
nal wavy layers.
4. Discussion
The present study found an improvement in th
adsorption of surfactants at an air liquid inte
face on addition of EO. The effects of EO o
minimum surface tension and stability were no
consistent for all surfactant formulations. Th
addition of EO was beneficial consistently o n
for film adsorption. A beneficial effect on all th
parameters studied was observed in the case
PCPEEO when compared with PCPE. This w
associated with a decrease in the size of the lipo
somes on addition of EO (8 10 mm in the case
P CP EE O a nd 20 30 mm size in t he ca se
PCPE).
The addition of EO, which contains eucalypto
as one of its main components, could promo
dissolution of large micelle structures and cau
fusion of micellar contents. Such properties hav
been observed in the case of hydrophobic surfa
tant specific proteins causing more homogenou
behavior of phospholipid suspensions (Rana
al., 1993). A similar phenomenon may account fo
the improved adsorption of the phospholipids o
addition of EO. Microscopically, the surfactan
in the presence of EO formed open membranou
structures, which could represent this proces
This is in accordance with the finding of Sasa(1990) that open membranous structures are fun
tionally beneficial when compared to close
structures.
The small sized, easily fracturable liposomes
PCPEEO could perhaps account for its superio
in vitro performance. This is in partial agreeme
with the findings of Denizot et al. (1991) th
small sonicated liposomes show faster adsorptio
a t a n a i r liquid interface than the polydisper
larger liposomes. Though our study also foun
small liposomes of PCPEEO to be functionalbeneficial, it did not seem to be a necessity fo
adequate adsorption. Open membranous stru
tures, regardless of size, appeared to be favorab
for adsorption. However, the small size appeare
to be related to better surface tension reduction
stability and re-spreading.
Fig. 6 (A) depicts a liposome of PCPE whereas
Fig. 6 (B), (C), and (D) depict structures in the
presence of EO. Fig. 6 (B) shows a PCEO lipo-
some, which is organized into wavy membranous
folds. Similarly, Fig. 6 (C) depicts the partially
fractured surface of a liposome of PCPE in the
presence of EO and the open membranous organ-isation of a totally fractured liposome of PCPG in
the presence of EO and 5 mM calcium is seen in
Fig. 6 (D). On comparing the ultrastructure of
PCPE and PCPEEO, it was observed that PCPE
formed large smooth liposomes 20 30 mm in size
whereas PCPEEO formed small liposomes barely
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PCPEEO was found to be comparable to Sur-
vanta in vitro with respect to surface tension
reduction and was superior to ALEC and Exosurf
with respect to all parameters compared mini-
mum surface tension, stability index and adsorp-
tion at Rmax. It also had a high re-spreading ratio,
as detected by the Wilhelmy balance study, com-
parable to that of ALEC and Exosurf. The im-proved adsorption and re-spreading, if extended
to in vivo conditions, could help in development
of a more ef ficient surfactant formulation which
could adsorb quickly to the air liquid interface of
the lungs and prevent collapse of the lungs by
lowering of surface tension. The improved re-
spreading would allow re-entry of surfactant ma-
terial into the interface with subsequent breaths
preventing a depletion of material from the inte
face due to losses. Further, the surface tension o
PC with EO and of PCPE with EO on adsorptio
at Rmax was B25 mN /m, which is similar to th
values observed for lung surfactant and its recon
stituted components (Ingenito et al., 2000). T h
presence of EO could perhaps help in the re-entr
of extra surfactant material from the surface assciated reservoir into the interface on expansion.
appears that PCPEEO may hold potential as
possible surfactant formulation.
However, we have not studied the compressibi
it y o f t he first compression monolayers in th
presence of EO, another important parameter fo
effective function. Furt her studies in a leak fr
captive bubble surfactometer would be inform
Fig. 6. Effect of EO on ultrastructure of surfactants. (A) depicts the ultrastructure of a liposome of PC:PE, 2:3. (B), (C) and (D
show the structures in the presence of EO. A liposome with wavy membranous folds is seen in (B) on addition of eucalytpus oil
DPPC. In (C), the structure of PCPE 2:3 in the presence of EO is seen. The liposomes are much smaller than the ones of PCP
The open membranous structure of PCPG with EO in the presence of 5 mM calcium is shown in (D).
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150
tive in this regard. Thus, the addition of EO (1%)
to PCPE (2:3) resulted in a favorable surfactant
formulation in vitro. It was found to be a promis-
ing candidate for possible exogenous surfactant
therapy in R DS based on its in vitro properties. It
is to be remembered that in vitro studies do not
necessarily provide an accurate determination of
in vivo exogenous surfactant efficacy due to in-
hibitory effects of plasma proteins, the in vivo
metabolism of the exogenously administered sur-
factant and inability to model the complex envi-
ronment of the lungs in vitro. Thus, one must be
cautious while extending these findings to in vivo
conditions. Further research in the form of animal
trials is required. Also, EO has never been used in
neonates and its safety remains to be established.
Though very low doses have been of EO have
been used in this study, far below the doses
described to have toxic effects 2 5 m l (Tibballs,
1995; Day et al., 1997) and Webb and Pitt (1993)
failed to find any toxic effects in children under 14
yr age even on oral ingestion of more than 30 ml
of the oil, this requires to be further con firmed.
In the event of its success in animal trials and
its passing the toxicity tests, PCPEEO could be a
promising surfactant formulation, which would be
inexpensive and could be beneficial to many ba-
bies in developing countries who are otherwise
unable to afford the present day surfactants.
Acknowledgements
We would like to thank Prof. S. Major for
extending the facility of the LB trough in the Thin
Films Laboratory, Department of Physics, Indian
Institute of Technology, Bombay, India. One of
the authors (R.B.) is very grateful to Dr. N.S.
Morton for having had the opportunity to con-
duct the surfactometer experiments in the Steroid
Laboratory of the Department of Child Health,
Royal Hospital for Sick Children, Glasgow, Scot-land, UK. Our sincere thanks to Prof. A. Wilkin-
son, Oxford University, UK , for his help and
encouragement which made this work possible.
We would also like to extend our deep gratitude
to Prof. R.R. Puniyani of the School of Biomedi-
cal Engineering, Indian Institute of Technology,
Bombay, India, for his fruitful suggestion
throughout the course of this study. The funds fo
the research trip to UK were partly met by th
J.N. Tata Endowment for The Higher Educatio
of Indians.
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