in vitro evaluation of surfactants with eucalyptus

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  • 8/14/2019 In Vitro Evaluation of Surfactants With Eucalyptus

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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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    (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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    146

    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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    14

    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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