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R Peslin

Publications and source records attributed to R Peslin.

At least 73 records · Page 4Linked to original sources
PubMed1993

Respiratory mechanics studied by forced oscillations during artificial ventilation.

Potential advantages of the forced oscillation technique over other methods for monitoring total respiratory mechanics during artificial ventilation are that it does not require patient relaxation, and that additional information may be derived from the frequency dependence of the real (Re) and imaginary (Im) parts of respiratory impedance. We wanted to assess feasibility and usefulness of the forced oscillation technique in this setting and therefore used the approach in 17 intubated patients, mechanically ventilated for acute respiratory failure. Sinusoidal pressure oscillations at 5, 10 and 20 Hz were applied at the airway opening, using a specially devised loudspeaker-type generator placed in parallel with the ventilator. Real and imaginary parts were corrected for the flow-dependent impedance of the endotracheal tube; they usually exhibited large variations during the respiratory cycle, and were computed separately for the inspiratory and expiratory phases. In many instances the real part was larger during inspiration, probably due to the larger respiratory flow, and decreased with increasing frequency. The imaginary part of respiratory impedance usually increased with increasing frequency during expiration, as expected for a predominately elastic system, but often varied little, or even decreased, with increasing frequency during inspiration. In most patients, the data were inconsistent with the usual resistance-inertance-compliance model. A much better fit was obtained with a model featuring central airways and a peripheral pathway in parallel with bronchial compliance. The results obtained with the latter model suggest that dynamic airway compression occurred during passive expiration in a number of patients. We conclude that the use of forced oscillation is relatively easy to implement during mechanical ventilation, that it allows the study of respiratory mechanics at various points in the respiratory cycle, and may help in detecting expiratory flow limitation.

Adult↗
PubMed1993

[Comparison of bronchodilator effects and site of action of fenoterol and ipratropium in chronic obstructive bronchitis].

There is no lack of data in the literature reporting on the efficacy of different bronchodilators. However, the discussion concerning the superiority of one bronchodilator over another in patients with chronic bronchitis and airflow obstruction is, and remains, a controversial subject. This has been particularly so since the perfection of synthetic anticholinergics delivered by inhalation without any side-effects. The aim of the present work is to compare the bronchodilator effects of a sympathomimetic, fenoterol (Berotec), and of an anticholinergic, ipratropium bromide (Atrovent), compared to a placebo in twelve unselected chronic bronchitics who had airflow obstruction and were in a stable clinical state. The bronchodilator effect of the two drugs was judged at the same time by variations on forced expired volume (FEV1) which was taken as a reference value, and of the maximum mid-expiratory flow (MEF) measured by spirography and also the variations of pulmonary resistance (delta Rrs) measured by the forced oscillatory method. The comparison of these indices enables the site of action of these agents to be specified. The dose response curve and the duration of action over six hours was assessed for each of the three agents. These were administered in succession and at random over three days by inhalation using an inhalation chamber. All the patients who were included were capable of producing a bronchodilator response but two of them responded only to one agent. The change in the FEV1 was comparable with the two active products. The change in MEF (an index of peripheral airways) was significantly greater following ipratropium.(ABSTRACT TRUNCATED AT 250 WORDS)

Administration, Inhalation↗
PubMed1992

Mechanical properties of the upper airway wall in children and their influence on respiratory impedance measurements.

The upper airway wall impedance (Zuaw) may be responsible for a large artifact in the measurement of respiratory system impedance (Zrs) in children. In 17 normal children aged 3.5-13 years Zuaw and Zrs were estimated by varying transrespiratory pressure directly at the mouth (conventional method: Z1) and around the subject's head (head generator method: Z2) from 4 to 32 Hz. Zrs and Zuaw were calculated from Z1 = Zrs.Zuaw/(Zrs+Zuaw) and Z2 = Zrs (1 + Zp/Zuaw), where Zp is the impedance of the pneumotachograph. From the real and imaginary part of Z1, Z2, Zrs, and Zuaw, the corresponding resistance, inertance, compliance and resonant frequency were calculated assuming simple RIC models. No significant difference was found between the mean +/- SE of parameters derived from Zrs (respectively, 6.8 +/- 0.4 cmH2O.L-1.s, 0.034 +/- 0.001 cmH2O.L-1.s2, 10.4 +/- 0.8 m.cmH2O-1, 9.1 +/- 0.3 Hz) and Z2 (6.8 +/- 0.4 cmH2O.L-1.s, 0.038 +/- 0.002 cmH2O.L-1.s2, 10.7 +/- 0.7 ml.cmH2O-1, 8.7 +/- 0.4 Hz). All but the compliance, derived from Z1 were significantly different (P less than 0.01) from those derived from Zrs (5.3 +/- 0.3 cmH2O.L-1.s, 0.008 +/- 0.001 cmH2O.L-1.s2, 11.9 +/- 1.2 ml.cmH2O-1, and 20.3 +/- 1.6 Hz). Respiratory resistance and compliance correlated significantly with height (r = -0.56 and 0.86, respectively), in contrast to upper airway wall resistance (Ruaw) and compliance (Cuaw). Ruaw (8.6 +/- 0.8 cmH2O.L-1.s), Cuaw (1.2 +/- 0.2 m.cmH2O-1), and upper airway wall inertance (0.030 +/- 0.004 cmH2O.L-1.s2) were close to those obtained by direct measurements in adults. The mechanical properties of the upper airway wall are responsible for a significant error in the measurement of Zrs by the conventional method in normal children. Most of the artifact may be corrected for by applying pressure around the child's head.

Biomechanical Phenomena↗
PubMed1992

Evaluation of the multiple linear regression method to monitor respiratory mechanics in ventilated neonates and young children.

A potentially useful method to monitor respiratory mechanics in artificially ventilated patients consists of analyzing the relationship between tracheal pressure (P), lung volume (V), and gas flow (V) by multiple linear regression (MLR) using a suitable model. Contrary to other methods, it does not require any particular flow waveform and, therefore, may be used with any ventilator. This approach was evaluated in three neonates and seven young children admitted into an intensive care unit for respiratory disorders of various etiologies. P and V were measured and digitized at a sampling rate of 40 Hz for periods of 20-48 s. After correction of P for the non-linear resistance of the endotracheal tube, the data were first analyzed with the usual linear monoalveolar model: P = PO + E.V + R.V where E and R are total respiratory elastance and resistance, and PO is the static recoil pressure at end-expiration. A good fit of the model to the data was seen in five of ten children. PO, E, and R were reproducible within cycles, and consistent with the patient's age and condition; the data obtained with two ventilatory modes were highly correlated. In the five instances in which the simple model did not fit the data well, they were reanalyzed with more sophisticated models allowing for mechanical non-homogeneity or for non-linearity of R or E. While several models substantially improved the fit, physiologically meaningful results were only obtained when R was allowed to change with lung volume. We conclude that the MLR method is adequate to monitor respiratory mechanics, even when the usual model is inadequate.

Airway Resistance↗
PubMed1992

Pulmonary mechanics after cardio-pulmonary transplantation, an experimental study.

An experimental model was developed in pigs (weight: 25 +/- 2 kg), to evaluate pulmonary mechanics during the first 2 h of reperfusion following heart-lung transplantation. We studied two groups with three transplantations each: group A (45 min of preservation) and group B (6 h of preservation). After rinsing out the heart-lung mass by the injection of a cold intracellular solution (K+ = 115 mEq/l) into the aorta and the pulmonary artery, the organs were removed and conserved in a cold environment (0.5 degrees C). The orthotopic heart-lung transplantation was carried out using extra-corporeal circulation. Pulmonary mechanics were evaluated before and after transplantation by measuring the pulmonary compliance (C), and the aero-dynamic resistance (R) with an interrupted air flow technique. [table: see text] The duration of ischaemia appeared to be a pernicious factor in cardiopulmonary function. In all cases, the protection protocol of the heart-lung block had allowed a cutting-off of the cardiorespiratory assistance. However, there were major pulmonary mechanical perturbations, associated with a reduction in the pulmonary compliance and a very important increase in the aerodynamic resistance.

Animals↗
PubMed1992

Ventilatory dynamics in children and adults during sinusoidal exercise.

The ventilatory response to sinusoidally varying exercise was studied in five adults and seven prepubertal children to determine whether the faster kinetics of ventilation observed in children during abrupt changes in exercise intensity remained more rapid when exercise intensity varied continuously. Each subject exercised on a cycle ergometer first against a constant load and then against a load fluctuating over six different periods ranging from 0.75 to 10 min. The pedal rate was kept constant for all loads. The inspiratory minute ventilation was determined breath-by-breath. Amplitude (A) and phase angle (phi) of the fundamental component and the first harmonics of the ventilatory response were calculated by Fourier analysis for an integer number of waves for each period. From the relationship between A, phi and frequency, dynamic parameters of a first order model with and without delay were compared between adults and children. Firstly we found that the ventilatory time constant was significantly faster in children: 49.7 (SD 9.1) s vs 74.6 (SD 11.1) s (P less than 0.01). Secondly, the change in A and phi with the frequency was not however characteristic of a first order system without delay in most of the subjects (phi greater than 90 degrees for the shorter periods). Thirdly, even when the ventilatory control system was described as a first order model with a positive delay, time constants remained significantly shorter in children: 45.6 (SD 5.7) s vs 67.4 (SD 13) s (P less than 0.01). The ability to increase ventilation faster in children appeared to be a characteristic of the ventilatory control system during exercise independent of the type of drive used.

Adolescent↗
PubMed1992

Changes in inspired gas composition and experimental bronchospasm in the rabbit.

In clinical practice, bronchospasm could be facilitated by hypoxia and by hypercapnia. In this study we assessed the influence of breathing a hypoxic (FIO2 = 0.10) or a hypercapnic (FICO2 = 0.08) gas mixture on the response to nebulized histamine (2% solution for 5 min) in anesthetized, tracheotomized, paralyzed and mechanically ventilated rabbits. Total respiratory resistance (Rrs) and elastance (Ers) were derived by least-square analysis from the relationship between tracheal pressure and flow. Control values of Rrs were larger during hypoxia and hypercapnia than in air while the values of Ers were similar. The absolute change in Rrs after histamine was similar in air and hypoxia, and larger in hypercapnia. The relative change, however, was smaller in hypoxia than in the two other conditions. Ers was also substantially increased by histamine and, contrary to Rrs, remained high 60 min after the aerosol. The results suggest: (1) that both hypoxia and hypercapnia increase airway resistance but do not change tissue properties; (2) that the response to histamine is depressed by hypoxia; (3) that a substantial part of the immediate response, and most, if not all, of the residual response after 60 min is due to changes in lung tissue viscoelastic properties.

Airway Resistance↗
PubMed1992

Respiratory transfer impedance and derived mechanical properties of conscious rats.

A setup is described for measuring the respiratory transfer impedance of conscious rats in the frequency range 16-208 Hz. The rats were placed in a restraining tube in which head and body were separated by means of a dough neck collar. The restraining tube was placed in a body chamber, allowing the application of pseudorandom noise pressure variations to the chest and abdomen. The flow at the airway opening was measured in a small chamber connected to the body chamber. The short-term reproducibility of the transfer impedance was tested by repeated measurements in nine Wistar rats. The mean coefficient of variation for the impedance did not exceed 10%. The impedance data were analyzed using different models of the respiratory system of which a three-coefficient resistance-inertance-compliance model provided the most reliable estimates of respiratory resistance (Rrs) and inertance (Irs). The model response, however, departed systematically from the measured impedance. A nine-coefficient model best described the data. Optimization of this model provided estimates of the respiratory tissue coefficients and upper and lower airway coefficients. Rrs with this model was 13.6 +/- 1.0 (SD) kPa.l-1.s, Irs was 14.5 +/- 1.3 Pa.l-1.s2, and tissue compliance (Cti) was 2.5 +/- 0.5 ml/kPa. The intraindividual coefficient of variation for Rrs and Irs was 11 and 18%, respectively. Because most of the resistance and inertance was located in the airways (85 and 81% of Rrs and Irs, respectively), the partitioning in tissue and upper and lower airway components was rather poor. Our values for Rrs and Irs of conscious rats were much lower and our values for Cti were higher than previously reported values for anesthetized rats.

Airway Resistance↗
PubMed1992

Respiratory mechanics studied by multiple linear regression in unsedated ventilated patients.

Respiratory mechanics during artificial ventilation are commonly studied with methods which require a specific respiratory pattern. An alternative is to analyse the relationship between tracheal pressure (P) and flow (V') by multiple linear regression (MLR) using a suitable model. The value of this approach was evaluated in 12 unsedated patients, mechanically-ventilated for acute respiratory failure, and most with a history of chronic obstructive or restrictive respiratory disease. After correction for the non-linear resistance of the endotracheal tube, the data were analysed with the linear first order model: P = P0 + E.V + R.V' where E and R are total respiratory elastance and resistance, and P0 is the static recoil pressure at end-expiration. After exclusion of the cycles which clearly exhibited muscular activity, a good fit was observed in 25 out of 36 records (relative root-mean-square error less than 10%); the values of E and R were reproducible within cycles, and consistent with the patient's condition and the ventilatory mode. The intrinsic positive end-expiratory pressure (PEEPi), as derived from P0 and the applied PEEP, averaged 1.1 +/- 1.0 hPa. Using more sophisticated models, allowing for mechanical non-homogeneity or non-linearity of R or E, rarely improved the fit and often provided unrealistic data. In several subjects the discrepancy between the data and the first order model was consistent with expiratory flow limitation, which may severely impair the analysis. We conclude that, except in the case of expiratory flow limitation, the method is useful for routine clinical use and better implemented with the simple linear model.

Aged↗
PubMed1992

Within-breath variations of forced oscillation resistance in healthy subjects.

Respiratory resistance (Rrs) was measured by the forced oscillation technique at 10, 20 and 30 Hz in 54 healthy subjects. The sinusoidal pressure oscillations were applied around the head, rather than at the mouth, so as to minimize transmural pressure across extrathoracic airway walls and the corresponding artefact (Peslin et al., J Appl Physiol, 1985, 59, 1790-1795). The flow (V') and volume (V) dependences of Rrs during the respiratory cycle were analysed by least square regression according to: Rrs = K1 + 2.K2.[V']#- K3.V, where K1 and K2 are Rohrer's constants, and where K3 expresses the (negative) volume dependence of Rrs. The analysis was made separately on the inspiratory and expiratory phases. A good fit was usually found between the data and the model, with a root-mean-square error averaging 15% of the mean Rrs at 10 Hz. At all frequencies K2 and K3 were substantially and significantly larger, and K1 slightly lower during expiration than during inspiration. Rrs, K1 and K3 were minimum at 20 Hz, while K2 exhibited a strong positive frequency dependence. The decrease of Rrs from 10 to 20 Hz was entirely explained by the variations of its linear component, and its increase from 20 to 30 Hz was largely due to its flow dependent component. Both the phasic variations and the frequency dependence of the coefficients suggest that the model is purely descriptive and that coefficients K2 and K3 reflect a number of phenomena, including the variations in glottic aperture during the respiratory cycle.

Adult↗
PubMed1991

Viscoelastic properties of rabbit lung during growth.

Viscoelasticity of air-filled isolated lungs of 1-120 day old rabbits was studied at a mean transpulmonary pressure (P1) of 0.65 kPa by measuring: (1) their stress relaxation (SR) following step volume changes (delta V) corresponding to 5% of the vital capacity; (2) their resistance (R1) and elastance (E1) during sinusoidal cycling at 11 frequencies (f) ranging from 0.01 to 0.65 Hz. SR data were analyzed by least-square regression using Hildebrandt's logarithmic model (Hildebrandt, J. (1970) J. Appl. Physiol. 28: 365-372): delta P1/delta V = A - B.log(t) where A is an index of elastance, and B/A is a measure of viscoelasticity. Coefficients A and B were also obtained from R1 and E1 according to: R1 = B/9.2 f and E1 = A + 0.25 B + B.log(2 pi f). Elastance corrected for lung weight increased by 40% between day 1 and days 3-7, and decreased thereafter to reach 30% of its initial value in 120 day old rabbits. B/A ratios also demonstrated an initial rise, followed by a progressive decrease. Values of B/A computed from R1 and E1 were similar to those derived from SR data in 1 day old rabbits, but were 20-30% larger in older animals, which indicates the presence of an additional rate-independent dissipation during flow. Total internal dissipation during cycling varied little with frequency; it was largest in 3-7 day old animals where it represented 20% of the stored elastic energy.

Animals↗
PubMed1991

[Effect of the association propofol-alfentanil on bronchial resistances in asthmatic patients].

The bronchial resistances in 17 patients scheduled for ENT surgery were studied during general anaesthesia carried out with propofol and alfentanil. There were nine controls, all free from any allergic pathology. The other eight had bronchial hyperreactivity, with clinical asthma (one or two crises a month) treated with bronchodilators. Two had a complete Fernand-Widal syndrome, and the remaining six documented allergic asthma. All the patients were premedicated with hydroxyzine 2 mg.kg-1 orally on the eve of surgery, and two hours beforehand. Those patients who were on bronchodilators were given their drugs as usual with the premedication. Because bronchial resistances were measured with the patient breathing spontaneously (forced oscillation technique), induction was carried out in two steps, first with propofol 1.5 mg.kg-1, followed, two minutes later, by alfentanil 7 micrograms.kg-1. Once the bronchial resistances had been assessed the patient was given a further 2 mg.kg-1 dose of propofol, and alfentanil 40 micrograms.kg-1. The patient was then intubated, and anaesthesia maintained with propofol 9 mg.kg-1.h-1, and alfentanil 15 micrograms.kg-1 every fifteen minutes. In all, bronchial resistances were measured on the day before surgery, after premedication but before the patient had been given any anaesthetic drug, two minutes after the first injection of propofol, two minutes after the first injection of alfentanil, and after extubation. There were no significant differences between the two groups. Despite the small number of patients included in this study, it would seem that hydroxyzine, propofol and alfentanil may be used safely in patients with hyperreactive bronchi.

Adult↗
PubMed1991

Confidence intervals of respiratory mechanical properties derived from transfer impedance.

Short-term intraindividual variability of the parameters derived from respiratory transfer impedance (Ztr) measured from 4 to 32 Hz was studied in 10 healthy subjects. The corresponding 95% confidence intervals (CIo) were compared with those computed from a single set of data (CIL) according to Lutchen and Jackson (J. Appl. Physiol. 62: 403-413, 1987). Ztr was analyzed with the six-coefficient model of DuBois et al. (J. Appl. Physiol. 8: 587-594, 1956), which includes airway resistance (Raw) and inertance (Iaw), tissue resistance (Rti), inertance (Iti), and compliance (Cti), and alveolar gas compressibility (Cg). The lowest variability was seen for Iaw (CIo = 11.1%), closely followed by Raw (14.3%) and Cti (14.8%), and the largest for Rti and Iti (24.6 and 93.6%, respectively). Using a simpler model, where Iti was excluded, significantly decreased the variability of Iaw (P less than 0.01) and Rti (P less than 0.05) but was responsible for a systematic decrease of Raw and Iaw and increase of Rti. Except for Raw with both models and Iaw with the simpler model, CIL was greater than CIo. Whatever the model, a high correlation between both sets of confidence intervals was found for Rti and Iaw, whereas no correlation was seen for Raw. This suggests that the variability of the former coefficients mainly reflects experimental noise, whereas that of the latter is largely due to biological variability.

Adult↗
PubMed1991

Airways impedance during single breaths of foreign gases.

The changes in airways resistance (Raw) and inertance (Iaw) during single inspirations of pure methane, helium, neon, and ethane at a flow of 0.1 l/s were measured in six healthy subjects by use of a forced-oscillation technique. Raw and Iaw were computed from respiratory transfer impedance obtained at a frequency of 20 Hz by applying pressure oscillations at the chest and measuring flow at the mouth with a bag-in-box system. Compared with the air data, the changes of Iaw after inhalation of 500 ml of gas averaged -41.1% with methane, -82.8% with helium, -25.8% with neon, and +4.8% with ethane. These changes were slightly less than the changes in gas density (-45%, -86%, -31%, and +5%, respectively). The inhaled volumes at which 50% of the changes had occurred (V50) did not differ significantly among gases and were approximately 100 ml. For Raw the data were more noisy than for Iaw; they were discarded in two subjects because of a strong and irreproducible volume dependence in air. Consistent differences were seen between the remaining subjects, one of whom exhibited a predominant viscosity dependence of Raw, one a predominant density dependence, and two an intermediate pattern. V50s were larger for Raw than for Iaw, indicating a more peripheral distribution of Raw. For Raw, V50s were lower with helium than with methane, in agreement with the notion that density-dependent resistance is located mainly in the large airways. The results suggest that some information on the serial distribution of Raw and Iaw may be derived from impedance measurements with foreign gases.

Adult↗
PubMed1991

Compared responses of rat lungs to step volume changes and to sinusoidal forcing.

Lung pressure-volume hysteresis of cat lungs has been found by Hildebrandt (J. Appl. Physiol. 28, 365-372, 1970) to be 20-50% larger than predicted from stress adaptation data on the basis of a viscoelastic model. We have reinvestigated this phenomenon in isolated rat lungs with a different approach, in which the approximation inherent to using a model is avoided : Lung transfer function was derived from the digitally-computed Laplace transform of the pressure decay following a step volume change and used to predict lung pressure-flow relationship in the frequency domain. The latter was expressed in terms of lung effective resistance (Rlc) and effective elastance (Elc), and compared to the observed values (Rl and El) in the frequency range 0.01-0.5 Hz. The measurements were made in 5 lungs at a transpulmonary pressure (Pl) of 0.5 kPa and in 5 others at a Pl of 0.8 kPa. Rl was found to be 23-41% larger than Rlc at Pl = 0.5 and 29-51% larger at Pl = 0.8. El did not differ significantly from Elc at Pl = 0.5 but was 14-28% larger at Pl = 0.8. These results are in good agreement with previous findings. The differences between Rl and Rlc are proportional to the reciprocal of frequency and, thus, correspond to a rate-independent dissipation. They are consistent with a yield stress of 3-6 Pa.

Animals↗
PubMed1991

Thoracic gas volume at functional residual capacity measured with an integrated-flow plethysmograph in infants and young children.

Thoracic gas volume (TGV) was measured with an integrated flow plethysmograph in 15 infants aged 2-34 months. End-expiratory (TGVe) and end-inspiratory (TGVi) airway occlusions were compared, after correction of TGV for the occluded volume above functional residual capacity (FRC). The relationship between pressure at the airway opening (Pao) and volume displaced from the box during airway occlusion (Vg) was studied numerically by: 1) an algorithm including a correction for the drift of Vg and linear regression analysis (LR); and 2) Fourier analysis of the signals (FFT). TGVe was significantly higher than TGVi (256 vs 237 ml, 20.4 (square root of residual variance; p less than 0.002). The correlation coefficient of the Pao-Vg relationship was slightly but significantly higher for TGVi than for TGVe: 0.9968 (0.9937-0.9995) vs 0.9947 (0.9840-0.9990) (means and range). No difference was observed between LR and FFT, although the intra-individual coefficient of variation was lower for LR than FFT: 5.2% (1.6-11.3) vs 7.9% (1.9-21.0) (means and range). Model simulations suggested that the difference between TGVe and TGVi could be mainly attributed to gas compression in the instrumental deadspace and upper airway wall motion and/or to uneven distribution of alveolar and pleural pressure associated with chest wall distortion.

Airway Resistance↗