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An important step in assessing childhood asthma is to evaluate the effects of bronchodilator inhalation on the airways. The FOT is increasingly used in children because it is noninvasive, requires little cooperation, and is performed during spontaneous breathing (1). It may be more easily performed than forced spirometry in some young patients, as no voluntary respiratory manoeuvre is necessary. The child only needs to breathe quietly through a mouthpiece connected to the FOT apparatus. A small pressure variation is applied at the airway opening, usually directly at the mouth where flow is measured (standard generator, SG). The mechanical Zrs is calculated as the pressure flow ratio. A significant drawback of SG is that some flow is diverted with cheek vibration (Fig. 1, top). The so called upper airway artifact is particularly significant when the Zuaw is small relative to Zrs (2,3), i.e. in the presence of airway obstruction (2) as well as in young children (4,5). A significant underestimation of Zrs measured by SG (ZrsSG) may result. Holding the cheeks may be insufficient to prevent this artifact (6). Alternatively, if pressure is varied around the subject's head (head generator technique, HG, Fig. 1, bottom), the transmural pressure across the cheeks is minimal, most of the upper airway wall motion is prevented and Zrs measured with HG (ZrsHG) is almost devoid of upper airway artefact (5,7). The technique has been applied to various settings, including the pediatric lung function laboratory (8,9). However, the HG set-up is cumbersome, available to a few laboratories and the configuration of the generator may decrease tolerance in younger children. Alternative ways to assess change in bronchomotor tone using FOT measurements would thus be particularly useful at this age.

Figure 1
figure 1

Simplified diagram of two variants of the forced oscillation technique. An oscillatory flow (arrow on left) is delivered by a pressure generator (loud speaker) through a flowmeter (f) to the child's respiratory system (arrow on right). (Top) With standard generator, pressure varied only at the airway opening induces flow in upper airway wall (vertical arrows), which does not reach the respiratory system. (Bottom) With head generator, pressure is applied around the child's head enclosed in a canopy, i.e. both inside and outside the upper airway wall. The pressure difference across the upper airway wall is thus cancelled, except for the small pressure drop due to f. Upper airway wall vibration (dotted vertical arrows) is minimized and most of the measured flow enters the respiratory system.

Farré et al. (10) have proposed a simple method to effectively circumvent the upper airway artifact when estimating the overall respiratory response to methacholine. The airway effect of the bronchomotor agent is computed as change in Ars, the reciprocal of Zrs, as explained below. We are not aware of any data on this method applied to estimating reversibility induced by a bronchodilator. The issue is of particular importance because these effects need to be estimated routinely in asthmatic children.

The aim of the present study was therefore to test whether the airway response to salbutamol may be assessed using the change in Ars in young children. If the hypothesis is correct, then SG should yield similar estimate of the bronchodilatory effect of salbutamol than HG, which is virtually free of upper airway artifact.

MATERIALS AND METHODS

Rationale.

The rationale for analyzing FOT data as change in Ars during methacholine challenge has been presented in details elsewhere (10). Briefly, owing to the parallel arrangement of the respiratory impedance devoid of upper airway artifact (Zrs*) and Zuaw, ZrsSG is expressed as:

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Using corresponding respiratory admittance (ArsSG and Ars*) and upper airway wall admittance (Auaw), eq. 1 may be written:

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Applying to describe baseline (subscript 1) and bronchodilation (subscript 2):

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ΔArsSG, the observed change, is given by:

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As only Ars* is expected to change significantly after bronchodilation, Auaw2 = Auaw1 and therefore:

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It should be pointed out that, while Zrs may be split into a resistive component (Rrs) and nonresistive component (reactance, Xrs), such is not the case of Ars. Then, Ars is less selective for airway resistance than Rrs, and ΔArs reflects changes in both resistive and nonresistive properties (elasticity, inertia) of the respiratory system.

Subjects.

The study includes 36 young children (19 boys) with a history of asthma, where lung function was evaluated at baseline and after salbutamol. Age ranged from 3.5 to 7.5 y (5.5 ± 1.1 y) and height from 98 to 135 cm (113 ± 9 cm). Bronchodilator therapy was discontinued more than 12 h before the study. As justified later on, the data were selected when, after salbutamol, both HG and SG showed a decrease in respiratory resistance (Rrs) and an increase or no change in Xrs. The protocol was approved by the committee for human subject protection in biologic research (Centre Hospitalier Universitaire de Nancy, France), explained to the child and his/her parents and informed consent was obtained.

Measurements.

Zrs measurements were performed using the Pulmosfor apparatus (SEFAM, Vandoeuvre, France) that is in conformity with the recommendations issued by a task force from the European Respiratory Society (1). The child wore a nose clip and breathed through a mouthpiece and bacterial filter connected to a Fleisch no. 1 pneumotachograph (Metabo, Epalinges, Switzerland). Sinusoidal pressure variation (1 hPa peak to peak) was applied at 12 Hz in two different ways: 1) around the subject's head enclosed in a translucent Plexiglas canopy (7) and 2) by connecting the loud speaker directly to the pneumotachograph, with the cheeks unsupported. In this configuration, fresh air was continuously flushed through the circuit to prevent CO2 accumulation. Pressure and flow signals were low-pass filtered at 32 Hz using analog filters and digitized at a sampling rate of 96 Hz. The breathing component in the signals was eliminated using a fourth-order Butterworth high-pass filter with a corner frequency of 6 Hz. The Fourier coefficients of pressure and flow were computed, Rrs and Xrs calculated oscillation cycle per oscillation cycle according to Navajas et al. (11). A filtering procedure was included to detect spurious data associated with rapid flow transients, low signal-to-noise ratio or glottis closure (12). Airflow, tidal volume, Rrs, and Xrs were displayed immediately after each acquisition to allow visual inspection and selection of the data, which were stored on disk. The data were reported in inspiration only so as to minimize variability resulting from change in glottis aperture (13) or flow limitation (14) during expiration.

The child was familiarized with the equipment, instructed to breathe calmly and regularly during trial measurements. Acquisitions lasting 30–45 s were then started using HG or SG and repeated immediately thereafter using SG or HG. The duration of the measurement allowed analyzing an average of 15–20 breaths.

Two puffs of salbutamol (200 μg, GlaxoSmithKline, Marly Le Roi, France) were delivered during tidal breathing through an inhalation chamber (Nespacer, Astra France, Monts, France) and the measurements were repeated as above 10 min thereafter.

Data analysis.

Absolute and relative change after salbutamol from baseline were computed on Rrs (ΔRrsSG, Δ%RrsSG, ΔRrsHG, Δ%RrsHG) and Zrs (ΔZrsSG, Δ%ZrsSG, ΔZrsHG, Δ%ZrsHG). The effect of salbutamol on Xrs was analyzed as absolute difference (ΔXrsSG, ΔXrsHG) and, since the value was frequently close to zero, as percentage of baseline Zrs modulus (Δ%XrsSG, Δ%XrsHG). The modulus of differences between salbutamol and baseline admittances was calculated (|ΔArsSG|, |ΔArsHG|) and also expressed as % of the corresponding Ars modulus at baseline (|ΔArsSG|%, |ΔArsHG|%). Statistical analysis was performed using ANOVA for repeated measurements and linear regression. Data are expressed as mean + SD; a p value <0.05 was retained as significant.

RESULTS

Impedance.

Zrs data obtained with HG and SG before and after salbutamol are reported in Table 1. It may be seen that RrsSG and ZrsSG are significantly lower than, respectively, RrsHG or ZrsHG (p < 0.0001) and ΔRrsSG and ΔZrsSG significantly smaller than, respectively, ΔRrsHG or ΔZrsHG (p = 0.0001). Relative changes described in Figure 2 also show significant underestimation of Δ%RrsSG compared with Δ%RrsHG (p = 0.0003) as well as Δ%ZrsSG compared with Δ%ZrsHG (p = 0.05). On the other hand, XrsSG is significantly more negative than XrsHG (p < 0.0001) and ΔXrsSG significantly larger than ΔXrsHG (p < 0.0001, Table 1). Accordingly, the change in Xrs as a fraction of the total respiratory impedance is expectedly larger for SG (16.5 ± 10.7%) than HG (2.4 ± 4.6%, p < 0.0001).

Table 1 Respiratory impedance (hPa.L −1 .s) of the study population (n = 36)
Figure 2
figure 2

The response to salbutamol is expressed as percent decrease in respiratory resistance and impedance from baseline (respectively, Δ%Rrs, Δ%Zrs) and modulus of increase in respiratory admittance as percentage from baseline (|ΔArs|%). Light columns: standard generator (SG); dark columns: head generator (HG). Note Δ%Rrs and Δ%Zrs are significantly lower with SG than HG (respectively, p = 0.0003 and 0.05) but |ΔArs|% is equivalent with both techniques.

Admittance.

The Bland and Altman plot shows no increase in the scatter of individual differences |ΔArsSG| – |ΔArsHG| when the corresponding mean increases (p = 0.25, Fig. 3) and the mean difference in |ΔArs| is 0.009 L.s−1.hPa−1 |ΔArsSG| and |ΔArsHG| are significantly correlated (r2 = 0.39, p < 0.0001, Fig. 4A). However, as suggested by Figure 3, |ΔArsSG| (0.0432 ± 0.0220 L.s−1.hPa−1) is significantly larger than |ΔArsHG| (0.0337 ± 0.0188 L.s−1.hPa−1, p < 0.0001). On the other hand, |ΔArsSG|% and |ΔArsHG|% are not different from each other (Fig. 2) and are also significantly correlated (r2 = 0.47, p < 0.0001 Fig. 4B).

Figure 3
figure 3

Bland and Altman plot shows no significant correlation between the difference |ΔArsSG| − |ΔArsHG| and the corresponding mean (|ΔArsmean|). Abbreviations as in Figure 2. Dotted lines indicate limits of agreement (+ and –2 SD).

Figure 4
figure 4

Significant correlation between (A) |ΔArsHG| and |ΔArsSG| in 36 subjects (r2 = 0.39, p < 0.0001) and (B) |ΔArsHG|% and |ΔArsSG|% (r2 = 0.47, p < 0.0001). Identity lines are shown.

The ability of Rrs, Ars, and Zrs to detect positive responses to salbutamol is compared between SG and HG in Figure 5, using percentage changes ranging from 15% to 40%. It may be seen that discrepancy between paired curves is most between RrsSG and RrsHG, least between ArsSG and ArsHG and intermediate between ZrsSG and ZrsHG.

Figure 5
figure 5

Rate of positive responses to salbutamol computed in 36 children at different decision levels for each parameter. Circle, Ars; square, Zrs; triangle, Rrs. Filled symbol, standard generator; open symbol, head generator. Note difference between SG and HG is largest with Rrs, smallest with Ars, intermediate with Zrs. Abbreviations as in Figure 2.

DISCUSSION

To the best of our knowledge, this is the first report on mechanical respiratory admittance change induced by salbutamol in children. The study indicates that SG and HG yield concordant estimates of |ΔArs| and |ΔArs|% with similar values for |ΔArsSG|% and |ΔArsHG|%, while |ΔArsSG| appears significantly larger than |ΔArsHG|.

The expected Zrs response to salbutamol includes a decrease in Rrs and, frequently, an increase in Xrs. These changes have repeatedly been documented in both healthy (15,16) and stable asthmatic children (1517). It was decided to include only data exhibiting a decrease in Rrs associated or not to an increase in Xrs because |ΔArs|, as modulus of a complex quantity, is sign less, thus does not indicate the direction of the change and may theoretically result from any combination of Ars1 and Ars2 (eq. 3–6). Therefore, an improvement in airway function would not be differentiated from a change of equivalent magnitude expressing a paradoxical effect of salbutamol. Although worsening of airway function by beta-adrenergic drugs is unlikely in the current clinical context and has been reported in occasional children with cystic fibrosis (18,19), involving spirometry rather than Zrs (20), we felt it mandatory, at least from a theoretical point of view, to discard any ambiguous |ΔArs| data. The upper airway artifact is expected to attenuate the magnitude of change in Rrs induced by a bronchomotor intervention but unlikely to completely abolish—let alone reverse—this change. Therefore, whenever RrsSG is observed to decrease after salbutamol, the role of |ΔArsSG|% would be to more accurately describe the amplitude of the response.

In the current study, the Bland and Altman plot (Fig. 3) indicates no systematic increase in the differences between SG and HG as the mean difference increases. The observed range for these limits of agreement (Fig. 3) and the scatter of data points in Figure 4 could be explained by the fact that Rrs and Xrs contributed differently to the measurement variability with HG and SG. In addition, the measurements were not carried out simultaneously and the effect of time was likely to add to the variability in these asthmatic children (21). The significant correlation between |ΔArsSG| and |ΔArsHG| described in Figure 4A is similar to that previously reported with data on induced bronchomotor tone (10). However, in the latter study, |ΔArsSG| was not statistically different from |ΔArsHG|, e.g. 0.0295 L.s−1.hPa−1 and 0.0327 L.s−1.hPa−1, respectively, at 10 Hz (10), while we reported a mean difference between |ΔArsSG| and |ΔArsHG| of 0.009 L.s−1.hPa−1. Methodological discrepancies exist between the two studies regarding the excitation signal (pseudo-random noise versus sine wave), the type of computation (fast Fourier transform versus oscillation per oscillation), the period of the respiratory cycle analyzed (whole breath versus inspiration). A different effect of salbutamol on inspiration and expiration resistance has been suggested in children (22) and this could explain the difference between the current results—analyzed in inspiration oscillation per oscillation—and those by Farré et al. (10) obtained on whole breaths by fast Fourier transform. Finally, some difference between |ΔArsHG| and |ΔArsSG| can be expected from the arrangement of Zuaw and the pneumotachograph. Indeed, with HG, these impedances are in parallel and some of the respiratory flow, shunted by airway walls, is not seen by the pneumotachograph (7). However, based on the current pneumotachograph impedance and Zuaw values estimated in children (4), the effect is likely to be minimal.

Whatever the reason for the difference between |ΔArsHG| and |ΔArsSG|, it is of interest that relative changes—which are the important quantities in practice—were significantly correlated (Fig. 4B) and not significantly different. |ΔArsSG|% should thus be equivalent to |ΔArsHG|% in evaluating the respiratory response to salbutamol. On the other hand, Δ%ZrsSG was found significantly smaller than Δ%ZrsHG, although the difference was less significant than for Δ%Rrs (Fig. 2). This expresses the fact that both reactive and resistive changes combine in Δ%Zrs, with more change in Xrs being detected by SG compared with HG. It should be noted that, for comparison purpose, measurements were performed with cheeks unsupported, so as to have similar upper airway impedance with both HG and SG. Holding the cheeks with SG would be likely to further decrease the difference between Δ%ZrsHG and Δ%ZrsSG.

|ΔArsSG|% appears particularly helpful in routine since the FOT is mostly used in the SG mode in children and the computation may easily be performed on any set of Zrs data. The current protocol was not designed for sensitivity and specificity studies. To assess the potential diagnostic value of |ΔArsSG|%, the rate of positive responses to salbutamol was computed at different decision levels for each parameter. Figure 5 shows the difference between SG and HG is marked for Rrs, intermediate for Zrs, and minimal for Ars. Thus, correcting for upper airway artifact by Δ%Ars is likely to improve the rate of identification of asthmatic children based on this estimate of their airway response to salbutamol. The improved value of |ΔArsSG|% in quantifying bronchodilation, compared with Δ%Zrs and Δ%Rrs, remains to be established in sensitivity/specificity studies. We have limited the study to the excitation frequency routinely used in our laboratory. Twelve hertz has been selected empirically for a long time because of the common observation of corrupted data in young asthmatics at lower frequencies. It must be noted that, as it minimizes the upper airway wall motion, the HG has the significant advantage to allow the use of frequencies a few hertz higher than the range recommended for SG (1). It is of interest that when using a pseudorandom noise (multi-frequency) excitation signal, the |ΔArs| response to methacholine in children was found to be independent of frequency with both SG and HG (10). Thus, a further potential advantage of |ΔArsSG|% would be to improve the signal-to-noise ratio by allowing higher excitation frequencies to be used without majoring the upper airway artiact.

The FOT has the potential to allow detailed description of mechanical respiratory characteristics from amplitude and phase of the pressure–flow relationship. Both Rrs and Xrs may be altered by a bronchodilator agent and, with conventional model interpretation, Rrs characterizes the flow resistive respiratory properties and apparent elasticity is described by Xrs (1,23,24). Such interpretation is of course not possible with |ΔArs|, which is contributed to by both resistive and reactive components. |ΔArs| in general characterizes the overall ease to respiratory flow and, at the particular resonant frequency, is equivalent to the change in respiratory conductance. On the other hand, interpreting changes in RrsSG and XrsSG induced by salbutamol, respectively, as change in bronchial diameter and as improvement in apparent elasticity is only theoretical, because the cheek artifact, not accounted for in the conventional model, modulates both responses (25). Therefore, the inconvenience of losing the ability to dissociate respiratory resistive and reactive effects of bronchodilator inhalation appears to be balanced by the fact that, in contrast to ΔRrs or ΔZrs, |ΔArsSG| is free of upper airway artifact. Here again, it should be stressed that conventional FOT parameters should be complemented with, rather than replaced by, |ΔArsSG| for a more accurate estimation of the bronchodilator effect.

Altogether, the current study indicates |ΔArsSG|% may be a valuable tool when evaluating reversibility of airway obstruction by bronchodilator therapy in asthmatic children. A qualitative assessment of Rrs and Xrs is necessary to insure the direction of the change. Further studies are needed in routine setting to assess the sensitivity and specificity of |ΔArsSG|% in detecting the response to bronchodilator in children with reference to conventional FOT parameters in a range of excitation frequencies.