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1 Department of Medical Informatics and Engineering, University of Szeged, H-6720 Szeged, Hungary; and 2 Department of Internal Medicine, University of Genoa, 16132 Genoa, Italy
THE RECENT
INTEREST IN SMALL animal models, which are particularly suitable
for genetic and translational studies on the pathophysiology of
bronchial asthma, has prompted the search for measurements of lung
function that are easy to implement and, if possible, noninvasive. In 1997, Hamelmann et al. (6)
proposed a plethysmographic method to assess airway responsiveness in
mice, which eventually gained wide popularity. The experimental setup
of this method is indeed extremely attractive: the animal is awake,
free to move, and restrained only in the sense that it is placed in the
plethysmograph. Only box pressure (Pb) is measured, and a
dimensionless parameter, called "enhanced pause" (Penh), is derived
from the shape of the Pb decay during expiration and the
ratio of the inspiratory and expiratory maxima of Pb. It
was found that Penh increased during bronchoconstriction and, in
anesthetized animals, correlated with pulmonary resistance, while it
was apparently independent of breathing frequency and pattern
(6). These observations led to the consideration of Penh
as a valid surrogate for pulmonary resistance.
The enthusiasm about this "unrestrained plethysmography" (UP),
however, was paralleled by some skepticism. This was because it was
unclear how a mechanical property could be estimated on the basis of a
single quantity not coupled to the respiratory system in any unique way
or, in terms of systems analysis, assessed without any measured or
standardized driving to which the response belongs. Mitzner and
Tankersley (10) questioned the key assumptions of UP and
also raised serious concerns about the appropriateness of its
experimental validation. In a review article on mouse models of airway
hyperresponsiveness, Drazen et al. (2) stressed the necessity to validate Penh with measurements of airway caliber based on
known physical principles. Peták et al. (12)
compared UP with the low-frequency oscillation technique in mice
exposed to 100% O2 and found a sharp increase in Penh,
whereas the airway resistance (Raw) decreased and the tissue parameters
remained unchanged. This implies that Penh may be completely unrelated to the mechanical properties of the lung but exclusively determined by
the breathing pattern, which may differ widely between different species and under different experimental conditions.
The lack of a theoretical basis and the questionable
specificity of UP have apparently been recognized by some of the
authors of the original publication (6), who included
standard (and invasive) measurements of respiratory mechanics in
subsequent studies (e.g., Ref. 1). It should also be noted
and appreciated that one of the authors of the original article is
involved in a critical reevaluation of UP also published in this issue
of the Journal of Applied Physiology (9), a
paper representing a laudable mission intended to avoid further
confusion about UP and to prevent its indiscriminate use in respiratory research.
The key issue about UP is the identification of the sources of
Pb, i.e., the physical processes occurring when an animal
is breathing unconditioned air and no signal but Pb is
available. There is substantial agreement (6, 10) that
Pb depends on 1) alveolar gas compression and
expansion to generate flow through the airways, and 2) tidal
volume (VT) plus any difference in temperature and humidity
between the inspired and alveolar gases. The chief object of
disagreement is the relative importance of these pressure sources, a
question that badly needed to be addressed quantitatively. Lundblad and
colleagues (9) point out that, when mice breathe spontaneously in a box where air is at room temperature and humidity, approximately two-thirds of Pb originate from gas
conditioning and approximately one-third from gas compression and
expansion. They also show that, under BTPS conditions, the
time integral of Pb over inspiration is accurately
predicted by a term containing Raw, lung volume, and VT,
which recalls the theory of plethysmographic measurement of Raw based
on energy dissipation (8). The conclusion is that, unless
lung volume and VT are measured or controlled, Penh will
not be suitable to characterize airway mechanics (6). It
is left to the reader to realize that this condition can hardly be
fulfilled with an unrestrained animal in a box and to return to the
reality of classic plethysmography as described by DuBois et al. in
1956 (3).
The need for noninvasive and repeatable measurements of airway
mechanics in experimental animals cannot be met by technically demanding and sophisticated, yet specific and sensitive methods such as
low-frequency oscillation technique (12). Meaningful mechanical variables can be obtained in restrained awake animals by
using a double-chamber plethysmograph and forced oscillations (7,
11) or a head-out plethysmograph to measure respiratory flow
(4). The article by Glaab et al. (5) in this
issue of the Journal of Applied Physiology describes the use
of head-out plethysmography in the assessment of bronchoconstrictor
responses in conscious rats. The method is based on the measurement of
midexpiratory flow (EF50) during tidal breathing and has
been validated by establishing the relationships between
EF50 in conscious and anesthetized animals and between
EF50 and pulmonary conductance (GL) in
anesthetized animals. Under a variety of experimental conditions,
EF50 and GL exhibited a fairly close
relationship, which justifies the authors' conclusion that
EF50 is an appropriate index of bronchoconstriction in a
rat model of asthma, although, as noted by Mitzner and Tankersley (10), "almost all respiratory mechanics variables show
qualitative correlations." Despite some differences between
EF50 and GL, probably reflecting different
sensitivities to airway and tissue components, this method has the
advantages of being relatively simple and based on meaningful physical quantities.
The present commentary is not intended to create a vacuum in
methodology by underlying the inadequacy of a technique and then to
propose another method with which to fill the vacuum. There is nowadays
a broad choice of experimental possibilities, including the few we
mentioned above, which yield rather similar respiratory quantities;
these techniques differ considerably as regarding the dimensions of
sophistication, confirmed validity, and the ease of instrumentation.
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REFERENCES
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FOOTNOTES |
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Address for reprint requests and other correspondence: Z. Hantos, Dept. of Medical Informatics and Engineering, Univ. of Szeged, Korányi fasor 9, H-6720 Szeged, Hungary (E-mail: hantos{at}dmi.u-szeged.hu).
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.
10.1152/japplphysiol.00526.2002
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