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1 Department of Chemical Engineering, University of Pittsburgh, and 2 Department of Pediatric Otolaryngology, Children's Hospital of Pittsburgh, Pittsburgh, Pennsylvania 15213
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ABSTRACT |
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Development of otitis media
has been related to abnormal Eustachian tube (ET) mechanics. ET is a
collapsible tube that is periodically opened to regulate middle ear
pressure and to clear middle ear fluid into the nasopharynx. The
ability to perform these physiological functions depends on several
mechanical properties, including the ET's opening pressure
(Popen), compliance (ETC), and hysteresis (
). In this
study, a previously developed modified force-response protocol was used
to determine ET mechanical properties after experimental manipulation
of the mucosal surface condition. Specifically, these properties were
measured in the right ear of six cynomologous monkeys under baseline
conditions after "washing out" the normal ET mucous layer and after
instillation of a pulmonary surfactant, Infasurf. Removal of the normal
mucosa did not significantly alter Popen but did result in
a decrease in ETC and
(P < 0.05). Treatment of the
mucosa with Infasurf was effective in reducing Popen and
increasing both ETC and
to baseline values (P < 0.05). These results indicate that the mucosa-air surface tension can affect the overall ETC and
properties of the ET. In addition, this
study indicates that surfactant therapy may only be beneficial in
patients with rigid or inelastic ETs (large Popen and low
ETC and
).
compliance; hysteresis; opening pressure; otitis media; elasticity
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INTRODUCTION |
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OTITIS MEDIA (OM) IS a common childhood disease that includes inflammation of the middle ear (ME) mucosa and an accumulation of fluid within the ME. By age 3, a significant number of children (33%) experience more than three episodes of OM (32). The persistence of OM often results in hearing loss, with possible effects on language acquisition, speech production, and social and educational development (31). The cost of treating persistent OM by medical and surgical procedures approaches $3 billion annually in the US (1). Although antibiotic treatment has proven effective in treating acute OM, the overuse of antibiotics has resulted in an increase in the prevalence of antibiotic resistance pathogens (5). In addition, surgical treatments, which include the placement of ventilating tubes in the tympanic membrane, require general anesthesia and are thus costly and distressing to children and their parents. The development of alternative treatment therapies for OM is, therefore, one of the most important, unresolved clinical problems in otology.
Although bacterial or viral infections and nasal allergies contribute to the onset of OM, the development of persistent OM is associated with a functional impairment of the Eustachian tube (ET) (2). The structure of the ET, which connects the ME with the nasal cavity, is similar to other respiratory airways in that the lumen of the tube is bounded by a fluid layer (the mucosa) and is surrounded by cartilaginous and muscular elements (2). Under normal conditions, the ET exists in a collapsed "closed" configuration that protects the ME from nasopharyngeal secretions. However, the ET is also responsible for maintaining ambient ME pressures and clearing ME fluid into the nasopharynx (2). These pressure-regulating and clearance functions require an open ET in which the resistance to air and fluid flow is minimal. ET dysfunction and the resulting disease complications can, therefore, develop when the tube is excessively patent or cannot be readily opened.
Flisberg et al. (6) were the first to suggest that the presence of surface tension-lowering substances (surfactants) might influence the function of the ET. Although the role of surfactant in ET has not been entirely determined, the presence and importance of these surface active substances in the lung have been well documented (33). The components of pulmonary surfactant, which include surface-active phospholipids and surfactant-associated proteins, are synthesized in the type II epithelial cells that line the alveolar walls (33). The presence of these surfactant components has been shown to influence the function and mechanics of the lung (19). Specifically, phospholipid surfactant molecules adsorb to the mucosal air-liquid interface and reduce the interfacial surface tension. This reduction in surface tension reduces the pressure required to inflate the lung, increases the compliance or flexibility of the lung, and stabilizes the mucosa to prevent airway collapse (3). In addition to these mechanical effects, hydrophilic surfactant proteins have been shown to enhance immunological functions in the lung (20). Premature infants suffering from respiratory distress syndrome (RDS) have not developed a mature surfactant system and must, therefore, be treated with exogenous surfactant to restore lung function. Several different surfactant systems, including a natural calf lung extract (Infasurf, ONY) as well as synthetically modified surfactants, have been developed and used to improve lung function and airway compliance in RDS infants (13).
Several studies have used a variety of biochemical techniques to document the presence of surfactant components in the ME-ET system of both animals and humans (21). Karchev et al. (16) found surfactant-producing cells in the dorsal section of the ET that are morphologically similar to the type II epithelial cells found in the lung. Recently, Paananen et al. (26) measured gene expression for several surfactant proteins in the porcine ET. In addition, Svane-Knudsen et al. (30) demonstrated that the quantity and composition of surfactant components in otologically healthy children are significantly different than the quantity and composition in children with OM. The presence of a sufficient quantity and quality of ET surfactant may therefore be an important determinant of ET function and mechanics.
ET mechanics.
The forces required to open the ET and maintain its patency will be a
function of several mechanical properties, including the elasticity of
the surrounding tissue and the surface tension of the fluid mucosa
layer. When collapsed, the ET is generally considered to be a
liquid-lined slit-like structure with a noncircular cross-sectional
shape (Fig. 1). However, histological
studies (28) have also demonstrated that this slit-like
structure can be buckled into several nearly circular lobes. Once this
structure is opened to airflow, increases in lumen pressure may result
in an opening of the slit-like structure and/or an opening of the circular lobes. To account for either situation, we have depicted a
generalized cross-sectional shape in Fig. 1 that can be used to
represent opening in a slit-like structure when the length-to-width ratio is large or opening in a circular lobe when the length-to-width ratio is 1. In either case, the surface tension of the liquid layer is
directed toward collapse of the ET lumen. The force required to
increase the lumen area [i.e., the translumenal pressure (
P)], must therefore overcome both surface tension and tissue elastic forces
(9). For a static system, the surface tension forces can
be related to the pressure drop across the air-liquid interface by
using a LaPlace's Law relationship, P
Pf = 
, where P is the internal lumen pressure, Pf is the
fluid pressure within the mucosa,
is the air-liquid surface
tension, and
is curvature of the mucosa-air interface. The tissue
elastic forces can be accounted for with a linear tube-law or
pressure-area relationship, Pf
Pext = EtissueA, where
Pext is the external pressure,
Etissue is the elastic modulus of the tissue,
and A is the cross-sectional lumen area (9).
The translumenal pressure [
P = P
Pext = (P
Pf) + (Pf
Pext) = 
+ EtissueA] will therefore be a
function of interfacial and tissue elastic properties [
P = f(
, Etissue)].
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P is related to the inflation of an opened ET, the initial
opening process is considerably more complicated. For example, as the
ME pressure is increased, a finger of air will penetrate into the ET,
separating its walls. At a critical pressure [i.e., the opening
pressure (Popen)], the liquid meniscus contained within
the lumen will rupture, and air will pass freely through an open ET.
Although the factors that determine this critical level are
complicated, the
P at the point of opening can be used to
approximate Popen = 
* + EtissueA*. Here,
* and A* are specific values at
the instant of opening and can only be determined from a detailed
analysis of this opening phenomena (9). Nonetheless,
Popen will be a function of both interfacial and tissue
properties (
, Etissue). In this study, we
focus on identifying the importance of interfacial mechanics by
introducing surface active agents that reduce
and should therefore
reduce the passive Popen of the ET.
In addition to Popen, the function of the ET has also been
associated with other mechanical properties, including ET compliance (ETC) or flexibility (15). ETC is defined in engineering
terms as the change in the cross-sectional area of the ET lumen for a
given change in
P (ETC = dA/d
P). Rigid or
inelastic ETs (low ETC) are difficult to open and thus might impair
ventilation and clearance functions. Conversely, ETs with high ETC,
often described as "floppy" ETs (2), may have impaired
protective functions. This lack of stiffness may also affect the
ability of the surrounding musculature to actively open the tube during
swallowing. ETC magnitude will be determined by the intrinsic stiffness
of the surrounding cartilage and muscular elements and the surface
tension forces at the air-liquid interface. Specifically, the applied
P must overcome surface tension and tissue elastic forces to produce a given change in A. An increase in
or
Etissue will result in a larger
P and,
therefore, a more rigid ET (small ETC). Conversely, a reduction in
Etissue or a reduction in
due to the
presence of surfactants will result in a smaller
P and a more
compliant/flexible ET (large ETC). Therefore, ETC will also be a
function of both interfacial and tissue elastic properties [ETC = f (
, Etissue)].
Another mechanical property that may influence ET function, but has not
previously been considered, is the ET's hysteretic nature. Hysteresis
occurs when the forces acting on the ET (i.e., pressure) are dissipated
such that they do not produce the same deformation (or cross-sectional
area) during inflation and deflation. Fredberg and Stamenovic
(8) have quantified hysteretic phenomena in lung tissue by
using a hysteretic modulus (
). Furthermore, these authors described
how surface tension hysteresis at the air-liquid interface caused by
the presence of pulmonary surfactants (
h) and the
viscoelasticity of the surrounding tissue (µtissue) can
both influence global hysteretic phenomena. Therefore,
will also be
a function of both interfacial and tissue mechanical properties [
= f(
, µtissue)].
The goal of the present study is to selectively alter the mucosal
surface condition to determine whether interfacial properties can
significantly affect global ET mechanical properties. Specifically, we
will quantitatively determine how removal of the normal ET mucosal
surfactant and the subsequent instillation of a natural pulmonary
surfactant extract (Infasurf) affects Popen, ETC, and
.
Although a study by Miura et al. (22) attempted to
determine the ability of surfactant to modify ETC, that study used a
nonphysiological surfactant and was based on a summary parameter that
is not consistent with the engineering definition of compliance. In
addition, ET
has not been specifically investigated. Therefore, the
present study uses a physiological surfactant (Infasurf) and measures ET mechanical properties with a modified force-response test previously developed by our research group (10). This testing
protocol is unique in that ET mechanical properties (ETC and
) are
determined by correlating pressure-flow (P-
) measurements with a
mathematical model of flow in a collapsible tube. ETC determined by
this protocol is therefore consistent with the engineering definition.
An accurate determination of how the mucosa-air surface tension and
surfactant administration affect ET mechanics may lead to a better
understanding of how surfactant therapy may be used clinically to treat
OM patients.
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MATERIALS AND METHODS |
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For this study, data were obtained from the right ears of six
cynomologous monkeys (Macaca fascicularis, 2-4 kg). The
monkey was chosen as the animal model since previous investigators
demonstrated that the operational biomechanics of monkey and human ETs
are nearly identical (4). All protocols used in this study
were approved by the Children's Hospital of Pittsburgh Animal Research and Care Committee. For each experiment, the monkey was sedated with 30 mg of ketamine and anesthetized with "monkey mix" (10 mg/kg
ketamine, 2 mg/kg xylazine, and 0.3 mg/kg acepromazine). The external
auditory canal was cleaned, and normal ME status was verified by using
tympanometry. Once a myringotomy was performed in the right tympanic
membrane, a probe with an integrated flow sensor and micropressure
transducer was hermetically sealed in the right external auditory
canal. All pressures were measured relative to the ambient atmospheric
pressure. As shown in Fig. 2, the
probe was connected to a syringe pump that delivered air at
specific flow rates. Continuous outputs from the flow and pressure sensors were routed to a microcomputer for visual display in real time
data storage and data processing using a HP VEE data acquisition routine (Agilent Technologies) (10).
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After each experimental manipulation described below, data were
obtained and analyzed in each animal according to the modified forced-response protocol previously developed in our laboratory (10). In this protocol, the syringe pump was used to
inflate the ME with ambient air at a flow rate of 5 ml/min until ET was forced open at Popen, as shown in Fig.
3A. After ET was opened, the
syringe pump was programmed to produce a sinusoidal flow rate between
5.0 and 23 ml/min with a period of 72 s. The pressure and flow
rate were measured simultaneously as a function of time until a steady
state, defined as a <5% change in the maximum and minimum pressure
between two successive oscillations, was obtained (Fig. 3A).
The magnitude of this oscillation cycle is based on steady-state flow
rates used in previous investigations (4), whereas the
oscillation frequency is small enough to ensure that air behaves like
an incompressible viscous fluid and large enough to ensure that the
test could be conducted in a reasonable amount of time
(12). Data for analysis consisted of the pressure and flow
rate during the final oscillation period, which was plotted as a
P-
hysteresis loop (see Fig. 3B). This P-
loop
was then correlated with a mathematical model of airflow in a
collapsible tube (solid line in Fig. 3B) to obtain ETC and
(12). This correlation technique, which is described
in the APPENDIX, is based on a least-square analysis and
resulted in correlation coefficients (r2) that
were consistently >0.95. Note that ETC and
are global parameters
and may therefore depend on both interfacial as well as tissue
mechanical properties. In general, the average slope of the P-
loop is inversely related to ETC (i.e., larger slope results in lower
ETC), whereas the area enclosed by the loop is directly related to
(i.e., larger area results in larger
). Execution of this protocol,
therefore, results in three primary parameters that describe the
mechanics of ET (Popen, ETC, and
).
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These mechanical parameters were determined by performing this modified forced-response protocol after various experimental manipulations. First, baseline mechanical parameters were determined in freshly perforated ears before any manipulation (Normal conditions). Second, the ME-ET system was rinsed with 37°C isotonic saline at 1 ml/min for 5 min. For this procedure, animals were placed in a prone position, and the ET lumen was washed by injecting saline into the ME via the hermetically sealed probe and collecting the washed fluid at the nasal orifice. Once the ET was rinsed, any residual fluid in the ME was cleared by subsequently introducing airflow at 5 ml/min for 2-3 min. After the normal ET mucosa had been disrupted in this manner, the mechanical parameters were measured via the testing protocol (Saline conditions). Finally, the ET lumen was treated with a calf lung surfactant extract, Infasurf, currently used to treat RDS infants. The surfactant solution was injected into the ME-ET system at 1 ml/min for 2 min, and the residue was collected at the nasal orifice. After this surfactant installation, residual ME fluid was again cleared with air at 5 ml/min for 2-3 min. Mechanical properties of the surfactant-treated ET were then measured with the testing protocol (Surfactant conditions). After these experimental manipulations, the probe was removed, and the external ear canal was cleaned with an alcohol solution to reduce the possibility of infection.
Mechanical parameters (Popen, ETC,
) were determined for
six animals under three treatment conditions: normal, saline, and surfactant. A within-subjects ANOVA was performed to document statistically significant differences among all treatment groups, whereas post hoc planned comparisons were used to document
statistically significant differences between individual treatment
groups. Significance for these tests was set at P < 0.05.
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RESULTS |
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Popen measured in each animal after a given
experimental manipulation is presented in Fig.
4. Mean Popen values measured
under each experimental condition are reported in Table
1. These mean Popen values
were significantly different (F = 27.8, P < 0.01). Post hoc between treatment comparisons
indicated that mean Popen measured under normal conditions
was not significantly different from mean Popen measured
after the ET mucosa had been rinsed in saline (P = 0.80). Mean Popen measured after surfactant instillation, however, was significantly lower than mean Popen measured
under both normal and saline conditions (P < 0.01).
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P-
loops measured in a typical subject during each
experimental condition are presented in Fig.
5. Only the mathematical correlations are
displayed for clarity. The P-
loop measured after the ET was
rinsed with saline had a larger slope and less loop area than the
P-
loop measured under normal conditions. Subsequent
administration of surfactant resulted in a slight decrease in the slope
of the P-
loop and an increase in the loop area. These
qualitative observations were quantified by analyzing each loop with
the mathematical model presented in the APPENDIX and
described in detail by Ghadiali et al. (12). This analysis
resulted in a quantitative measurement of the ETC and
parameters in
each animal for a given experimental manipulation. Mean values for these parameters under each experimental condition are reported in
Table 1. The variation of ETC between treatment groups is presented in
Fig. 6A. Mean ETC values were
significantly different (F = 4.11, P < 0.05). Between-treatment comparisons indicated that mean ETC under
saline conditions was significantly lower than mean ETC measured under
both normal and surfactant conditions (P < 0.05). In
addition, ETC measured under surfactant conditions was not
significantly different from ETC measured under normal conditions
(P = 0.48). The variation of
between treatment
groups is presented in Fig. 6B. Mean
values were also
significantly different (F = 8.55, P < 0.01). Between-treatment comparisons indicate that mean
measured
under saline conditions was significantly lower than mean
measured
under normal and surfactant conditions (P < 0.05). In
addition, mean
measured under surfactant conditions was not
significantly different from mean
measured under normal conditions
(P = 0.57).
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DISCUSSION |
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We measured several ET mechanical properties after flushing the ET
mucosa with saline and after the subsequent administration of a natural
pulmonary surfactant, Infasurf. These mechanical properties include
Popen, ETC, and
. These parameters were measured in six
cynomologous monkeys with the previously developed modified force-response technique. This technique, which is based on an engineering model of airflow in the ET, results in an accurate determination of global ET mechanical properties. Although both interfacial and tissue mechanical properties could affect these global
mechanical properties, our goal was to obtain a better understanding of
how disruption of the normal mucosal surface condition and treatment of
the mucosa with a pulmonary surfactant influences global ET mechanics.
Therefore, these experiments were designed to alter interfacial
properties without affecting the tissue mechanical properties.
Although washing of the ET mucosa with saline did not result in a
significant change in Popen, the instillation of Infasurf into the ET resulted in a reduction in Popen consistent
with a reduction in the mucosa-air surface tension. To interpret these results, which are consistent with similar measurements obtained in
gerbils (7), we consider the conceptual model for ET
opening shown in Fig. 1. In this model, Popen will be a
function of both
and Etissue. Specifically,
as discussed in the introduction, Popen = 
* + EtissueA*. Instillation of a
pulmonary surfactant that reduces
therefore results in a reduction
in Popen (see Fig. 4). These results are also consistent
with the ability of surfactants to reduce Popen or
inflation pressure in the lung as documented by using both ex vivo lung
models (23) and in vitro airway models (11). However, the normal vs. saline data in Fig. 4 indicate that native surfactant does not significantly contribute to Popen and
that, under normal conditions, Popen is mainly determined
by other factors, i.e., Etissue. Although native
surfactant may not influence Popen under normal conditions,
the fact that a pulmonary replacement surfactant significantly reduces
Popen may have important clinical consequences. For
example, patients with OM typically present with an inflamed ME mucosa
and consequently have high ET Popen due to an elevated
Etissue. Under these conditions, surfactant therapy could potentially reduce
and, therefore, reduce
Popen to normal values even if
Etissue were elevated. This paradigm was in fact
studied by Nemechek et al. (24), who found that Popen in normal ears was not significantly different from
Popen in inflamed ears treated with surfactant.
Although Popen may be an important factor, several other
mechanical properties, such as ETC and
, will also be important determinates of ET function. However, the influence of
and
surfactant on these properties has not been adequately studied. The
current study was therefore designed to provide new information with
respect to how surfactants influence ETC and
. Figure 6A
demonstrates that
can significantly affect ETC. Washing the ET
lumen with saline, which potentially removes native surfactant and thus
increases
, resulted in a decrease in ETC and thus a more rigid ET.
Note that, although this increase in
is large enough to alter ETC, it is apparently not large enough to alter Popen (see Fig.
4). In contrast, application of a pulmonary surfactant to the ET lumen, which decreases
, resulted in an increase in ETC to prewashing values and thus a more flexible ET. This inverse relationship between
and ETC can be understood by recalling the definition of ETC as the
change in cross-sectional area for a given change in
P (ETC = dA/d
P). As discussed in the introduction,
P will be a function of
interfacial and tissue mechanical properties:
P = 
+ EtissueA. By assuming constant tissue
properties (dEtissue/dA = 0) and
negligible surface tension hysteresis (d
/dA ~ 0), we can
express ETC = (
*d
/dA + Etissue)
1. Therefore, ETC is
inversely related to
when d
/dA > 0 (see Fig. 1). This
inverse relationship is consistent with surface-tension forces directed
toward collapse of the ET. Specifically, as
increases, surface
tension collapsing forces increase, requiring a larger applied pressure
to maintain lumen area, which results in a more rigid ET (lower ETC).
This inverse relationship is also consistent with previous studies in
the pulmonary system. Specifically, Buchanan et al. (3)
demonstrated that airway compliance increases on surfactant
administration (i.e., decrease in
).
In contrast to this inverse relationship, Miura et al.
(22) reported an opposite behavior in which an index of
compliance, known as the tubal compliance index (TCI), decreased when
decreased due to the application of a nonphysiological surfactant.
TCI was defined as the ratio of the flow resistance
(Rs) at two different flow rates. Specifically,
constant flow in an open ET was established, and resistance was
calculated as Rs = Ps/
s, where Ps is the steady-state pressure and
s is the applied flow
rate. TCI was then calculated as the resistance at a low flow rate
(
s of ~10 cm/min) over the resistance at a high
flow rate (
s of ~40 ml/min). Because the
resistance to airflow in the ET is an inverse function of the lumen
area, this parameter essentially measures the relative change in lumen
area for a given change in flow rate. However, the elastic nature of
the ET (i.e., ETC) is related to how much force must be applied to
produce a given deformation or change in lumen area. The relevant force
in this system is the applied pressure (
P), not the flow rate. TCI,
therefore, may not be an accurate measure of compliance since it does
not relate changes in lumen area (i.e., resistance) to changes in the
applied pressure. We believe that the results of the current study,
which utilizes an engineering definition of compliance (i.e., ETC = dA/d
P) and successfully predicts an increase in compliance with a
reduction in surface tension, are a more accurate representation of the influence of surfactant on ET mechanics.
Another potentially important mechanical parameter that can be
influenced by the presence of surfactants is the hysteretic nature of
the ET. As demonstrated by the arrows in Fig. 3B, pressures obtained during inflation (i.e., increasing flow rate) may be slightly
larger than the pressure obtain during deflation, resulting in a
P-
loop. These loops are similar to the pressure-volume (P-V)
loops observed in the lung. In this study, the area of the P-
loop was quantified with a global hysteretic parameter (
). Fredberg
and Stamenovic (8) demonstrated that
may be a function of surfactant-induced surface tension hysteresis (
h) and
viscoelastic tissue properties. In this study, we have focused on the
influence of
h by altering interfacial properties by
using a pulmonary replacement surfactant. Pulmonary surfactant's
ability to generate a significant loop area depends on several complex
physical properties, including differences in adsorption and desorption
rates (25) and the development of multiple surfactant
layers on the air-liquid interface (18). We have
demonstrated that the P-
loop area observed in normal ETs can be
eliminated by removing the native ET mucosal surfactant (see Fig.
6B). This behavior is consistent with observations in the
lung where significant P-V loop area is observed in lungs with a
functional surfactant system, whereas the P-V loop area in lungs
without a functional surfactant system is negligible (19).
Therefore, chemical components of ET surfactant likely contain the
complex physical properties known to exist in native pulmonary
surfactant and are required to produce significant loop area. In
addition, the instillation of a pulmonary surfactant into the ET
resulted in an increase in loop area, as measured by
, to normal
values. Krueger and Gaver (18) demonstrated that the
pulmonary surfactant used in the current study, Infasurf, was also
capable of producing these hysteresis loops in an in vitro model of
lung alveoli. Therefore, Infasurf contains the requisite physical
properties to maintain P-
hysteresis in the ET and P-V
hysteresis in the lung.
Several recent studies investigated the efficacy of surfactant therapy on the resolution of OM (17). These studies were conducted by inducing acute OM experimentally with a bacterial agent, administering surfactant on a periodic basis, and observing the resolution time. For this experimental model, surfactants were found to be effective in reducing the resolution time. Bacterial infections of the ME cause mucosal inflammation, which likely results in increased Popen, decreased ETC, and thus a dysfunctional ET. The current study demonstrates that treatment with surfactant restores ET function by reducing the mucosa-air surface tension and thus reducing the Popen and increasing the ETC or flexibility of the ET. Although surface-active substances may be helpful in resolving acute OM due to infection and inflammation, persistent OM can develop due to a variety of pathological conditions related to the structure of the ET. For example, Bluestone and Klein (2) demonstrated that persistent OM can develop when the ET is highly compliant or floppy. This hypercompliance can occur in young children who do not have a sufficient quantity of cartilage or in older patients with decreased cartilage cell density or a degraded intracellular matrix. This lack of stiffness may affect the ability of the surrounding musculature to actively open the tube during swallowing. Clearly, administration of surfactant under these conditions, which would further increase ETC, is counterindicated for the resolution of disease conditions. Successful treatment therapies may therefore depend on an accurate understanding of both the specific influence surfactant therapy can have on the mechanics of the ET and the mechanical state of a given patient's ET. Specifically, surfactant therapy may only be effective in patients with high Popen and low ETC.
Although we have demonstrated that surfactants and surface tension
properties significantly affect global ET mechanical properties, tissue
mechanical properties are also expected to play a critical role. The
potential contributions of these tissue properties could be
investigated by measuring Popen, ETC, and
after
paralysis of a surrounding muscle (tensor veli palatini). As a result,
this study would determine how an experimental reduction in tissue elasticity, Etissue, affects the overall
mechanics of the ET. Future studies should also focus on developing a
delivery system that is more practical than the ME instillation
technique used in this study. For example, the efficacy of
administering a nebulized or aerosolized surfactant via the nasal
cavity could be investigated. In addition, the pulmonary surfactant
used in this study (Infasurf) as well as other surfactants used
to treat RDS infants are relatively expensive and therefore might not
be a viable treatment for OM due to financial reasons. Therefore,
future studies should also include an investigation of how various
nonphysiological and synthetic surfactants affect ET mechanics.
Finally, as noted above, the use of surfactant as an alternative,
noninvasive treatment option for OM will require knowledge of a
patient's ET mechanics. Although the modified force-response technique
used in this study has also been implemented in a clinical setting,
this test requires a perforation of the tympanic membrane. Because
surfactant therapy is potentially an alternative to this surgical
procedure, future studies should investigate other less invasive means
of obtaining the ET mechanical properties investigated in this study,
i.e., Popen, compliance, and hysteresis.
In summary, we have investigated the influence of the mucosal surface
condition and the administration of a pulmonary surfactant on the
mechanics of the ET. Removal of the normal mucosal blanket, which
potentially removes native surfactant components, did not significantly
alter Popen but did significantly decrease both the ETC and
. Administration of a pulmonary surfactant (Infasurf) significantly
decreased Popen consistent with a reduction in
. In
addition, pulmonary surfactant's ability to reduce the surface tension
resulted in a significant increase in ETC and
to normal values.
Knowledge of how surfactant affects these mechanical properties has led
to a better understanding of which patients may benefit from surfactant
therapy, i.e., patients with large Popen and rigid ETs.
With the development of noninvasive testing protocols, effective surfactant delivery methods, and cheaper synthetic surfactants, the use
of surfactant therapy may become a practical alternative to standard
antibiotic and surgical treatments of OM.
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APPENDIX |
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The mechanical parameters (ETC and
) were determine by
analyzing experimental P-
measurements with the fluid-structure model of airflow in a collapsible tube shown in Fig.
7 (12). In this model, a
Poiseuille-type relationship is used to describe the pressure drop
along the ET in terms of the cross-sectional area
[A(t)], and the flow rate [
(t)]
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(1) |
(t) is fixed by protocol
(qm = 14 ml/min,
qa = 9 ml/min, and
= 2
/72 s),
P(t) is the ME pressure, Pd is the downstream pressure, µ is the viscosity of air, L is the length of
the collapsed segment, and
S is a hydraulic-geometric
shape factor, which is only a function of the cross-sectional
shape. The solid mechanics are described by a potentially
nonlinear pressure-area relationship
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(2) |
represent the global stiffness and
hysteretic properties of the ET, respectively, and
A2 is the shape-independent area defined as
A2(t) = A(t)/
S1/2. Note that the
mechanical parameters (Etube and
) are
independent of the cross-sectional shape such that the correlation
technique described below does not require a specific
S
value. This model also assumes no variations in cross-sectional area
along the length of the ET, i.e., A = A(t) only, as suggested by histological
measurements (29).
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We seek solutions to these equations for P(t) as a
function of Etube,
, and Pext.
These solutions, however, require an assumption regarding
Pd and the coefficient n. As described in detail
by Ghadiali et al. (12), setting Pd = 0 and
allowing n > 1 results in a numerical solution scheme.
A simpler analytical solution can also be obtained by setting
Pd = Pext and n = 1. Note
that these assumptions were only made to obtain an analytical solution and may not have any physiological significance. As demonstrated by
Ghadiali et al. (12), the choice of models (i.e.,
numerical or analytical) does not substantially affect the magnitudes
of the Etube and
obtained when these models
are correlated with experimental data. Therefore, the current study has
utilized the simpler analytical solution.
Given the Pd = Pext and n = 1 assumptions, Eqs. 1 and 2 can be solved
analytically for A2(t). With this
expression for A2(t), Eq. 1 can be used to generate a predicted pressure that will be a
function of Etube,
, and Pext.
For each experimental condition, a least-squares regression analysis is
performed by varying the three free parameters to obtain the best fit
between predicted pressure and the experimentally measured
P(t). This regression technique is able to capture the
experimentally observed P-
hysteresis (see Fig. 3B)
and consistently results in a correlation coefficient of
r2 > 0.95. As a result, we can
quantitatively estimate the ET's global elastic and hysteretic
properties, Etube, and
. Because compliance
is defined as dA/d[P(t)
Pext], we utilize Eq. 2 to specify ETC = 1/Etube. Note that this "lumped-parameter"
model utilizes global parameters ETC and
, which may depend on both interfacial and tissue mechanical properties. Therefore, this model is
not able to specifically identify the functional form of these
relationships, Etube = 1/ETC = f(Etissue,
) and
= f(µtissue,
h).
| |
ACKNOWLEDGEMENTS |
|---|
We thank Dr. Edmund Egan and ONY for providing Infasurf samples for use in this study and Dr. William Karanavas for assistance in developing and maintaining the forced-response system.
| |
FOOTNOTES |
|---|
This research is supported in whole or in part by a Children's Hospital of Pittsburgh Fellowship and a research grant from the National Institute for Deafness and other Communication Disorders (P01 DC-01260).
Address for reprint requests and other correspondence: S. N. Ghadiali, Dept. of Pediatric Otolaryngology, Children's Hospital of Pittsburgh, 3705 Fifth Ave. @ DeSoto St., Pittsburgh, PA 15213 (E-mail: ghadiali{at}pitt.edu).
The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.
June 7, 2002;10.1152/japplphysiol.01123.2001
Received 9 November 2001; accepted in final form 30 May 2002.
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