An aid in the diagnosis of malpositioned double-lumen tubes.
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Biomedical subjects
Publications and source records attributed to B A Simon.
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High-frequency ventilation (HFV) is a modality of mechanical ventilation which presents difficult technical demands to the clinical or laboratory investigator. The essential features of an ideal HFV system are described, including wide frequency range, control of tidal volume and mean airway pressure, minimal dead space, and high effective internal impedance. The design and performance of a high-frequency oscillatory ventilation system is described which approaches these requirements. The ventilator utilizes a linear motor regulated by a closed loop controller and driving a novel frictionless double-diaphragm piston pump. Finally, the ventilator performance is tested using the impedance model of Venegas [1].
To test the hypothesis that high-frequency ventilation (HFV) promotes lung stability we compared the temporal course of dynamic lung compliance changes after two inflations on HFV with those occurring on conventional mechanical ventilation (CMV) at two different lung volumes, specifically with and without 5 cmH2O positive end-expiratory pressure (PEEP). In our first set of experiments we ventilated six anesthetized paralyzed dogs first with CMV, then with HFV, then again with CMV using tidal volumes of 15 ml/kg at rates of 16-18 times/min for CMV and less than 90 ml and a rate of 15 Hz for HFV. In our second set of experiments we ventilated six dogs for 4 h, the 1st h with CMV at 0 cmH2O end-expiratory pressure, the 2nd h with CMV with 5 cmH2O PEEP, the 3rd h with HFV at the same mean pleural pressure, and the 4th h again with CMV with 5 cmH2O PEEP. We found the decreases in dynamic compliance with time following hyperinflations were similar on HFV and CMV (P greater than 0.5) at both lung volumes. With the lower lung volume the initial dynamic compliance following hyperinflation also tended to fall progressively from one hour to the next despite the inflations. However, with PEEP the initial dynamic compliance over successive hours tended to rise from one hour to the next. We found that changes in dynamic compliance were not necessarily reflected in the venous admixture or alveolar to arterial O2 partial pressure gradients. We thus conclude that lung stability in normal dogs is not improved during HFV, and blood gases cannot be used to predict compliance changes.
Studies and applications of high-frequency ventilation (HFV) are often performed under conditions of controlled mean airway pressure (Paw). In the present study we tested the assumption that controlling Paw adequately controls lung volume during HFV by investigating the relationship between a reliably measured Paw and the mean alveolar pressure (Palv) of the lungs during HFV of healthy dogs. We minimized the errors of Paw measurement due to the Bernoulli effect and various technical factors by appropriate choice of transducers, amplifiers, and measurement site. Palv was estimated by clamping the ventilator tube during oscillation and measuring the equilibration pressure of the lung and airways. Paw and Palv were determined as functions of frequency (8-25 Hz), tidal volume (60-90 ml), Paw (-5 to 12 cmH2O), and position of the animal (supine vs. lateral). We found that Paw could significantly underestimate Palv and that the degree of underestimation increased at higher frequencies, larger tidal volumes, and lower Paw. Shifting the animal from the supine to the lateral position greatly accentuated this effect. The elevation of Palv above Paw was seen to be a function of mean flow and largely independent of the frequency-tidal volume combination which produced the flow. A possible explanation of this pressure difference is that it results from differences in inspiratory and expiratory airway impedances, which in turn depend on airway geometry, compliance, lung volume, and expiratory flow limitation.
The orientation of membrane fragments into a lamellar array by a flat surface is analyzed. This analysis includes processes such as centrifugation and drying and physical effects due to membrane fragment steric interactions, finite size, elasticity, and thermal fluctuations. Several model calculations of optimal orientational order in multilayer membrane arrays are presented. The predictions of a smectic A model agree quantitatively with the measured spatial dependence of the fluctuations in layer orientation in a multilamellar arrays. A new technique, based in part on this analysis, for the preparation of well-oriented multilamellar arrays of natural and artificial membranes, isopotential spin-dry centrifugation, is described. The method involves the use of specially designed inserts for the buckets of a standard vacuum ultracentrifuge. The membrane fragments to be oriented are sedimented from solution or suspension onto a substrate of a convenient material which forms a gravitational isopotential surface at high g. Sedimentation is accompanied by removal of the suspending medium at high g to produce oriented films with a selected degree of solvation. In addition, a method is described whereby small solute molecules can be maintained in constant concentration with the membrane fragments during this process. Initial application of the method to the orientation of purple membrane fragments is described. The degree of orientation obtained in this system is evaluated using freeze-fracture and scanning electron microscopy, optical birefringence, linear dichroism, and microscopy.