Convective Gas Mixing Research Articles

Lung volume is a determinant of aerosol bolus dispersion.

The technique of inhaling a small volume element labeled with particles ("aerosol bolus") can be used to assess convective gas mixing in the lung. While a bolus undergoes mixing in the lung, particles are dispersed in an increasing volume of the respired air. However, determining factors of bolus dispersion are not yet completely understood. The present study tested the hypothesis that bolus dispersion is related, among others, to the total volume in which the bolus is allowed to mix--i.e., to the individual lung size. Bolus dispersion was measured in 32 anesthetized, mechanically ventilated dogs with total lung capacities (TLCs) of 1.1-2.5 L. Six-milliliter aerosol boluses were introduced at various preselected time-points during inspiration to probe different volumetric lung depths. Dispersion (SD) was determined by moment analysis of particle concentrations in the expired air. We found linear correlations between SD at a given lung depth and the individual end-inspiratory lung volume (V(L)). The relationship was tightest for boluses inhaled deepest into the lungs: SD(40) = 0.068 V(L) - 1.77, r(2) = 0.59. Normalizing SD to V(L) abolished this dependency and resulted in a considerable reduction of inter-individual variability as compared to the uncorrected measurements. These data indicate that lung size influences measurements of bolus dispersion. It therefore appears reasonable to apply a normalization procedure before interpreting the data. Apart from a reduction in measurement variability, this should help to separate the effects on bolus dispersion of altered lung volumes and altered mixing processes in diseased lungs.

Dispersion of 0.5- to 2-micron aerosol in microG and hypergravity as a probe of convective inhomogeneity in the lung.

We used aerosol boluses to study convective gas mixing in the lung of four healthy subjects on the ground (1 G) and during short periods of microgravity (microG) and hypergravity ( approximately 1. 6 G). Boluses of 0.5-, 1-, and 2-micron-diameter particles were inhaled at different points in an inspiration from residual volume to 1 liter above functional residual capacity. The volume of air inhaled after the bolus [the penetration volume (Vp)] ranged from 150 to 1,500 ml. Aerosol concentration and flow rate were continuously measured at the mouth. The dispersion, deposition, and position of the bolus in the expired gas were calculated from these data. For each particle size, both bolus dispersion and deposition increased with Vp and were gravity dependent, with the largest dispersion and deposition occurring for the largest G level. Whereas intrinsic particle motions (diffusion, sedimentation, inertia) did not influence dispersion at shallow depths, we found that sedimentation significantly affected dispersion in the distal part of the lung (Vp >500 ml). For 0.5-micron-diameter particles for which sedimentation velocity is low, the differences between dispersion in microG and 1 G likely reflect the differences in gravitational convective inhomogeneity of ventilation between microG and 1 G.

Increased fine particle deposition in women with asymptomatic nonspecific airway hyperresponsiveness.

Previous studies suggest that lung function tests using monodisperse aerosols can help to identify early stages of lung diseases. We investigated intrapulmonary particle loss and aerosol bolus dispersion-a marker of convective gas transport-in 32 women with asymptomatic nonspecific bronchial hyperresponsiveness (BHR) compared with 60 women without BHR. Deposition of inhaled particles (0.9 micrometer mass median aerodynamic diameter [MMAD]) was calculated from particle losses of inhaled aerosol boluses consisting of di-2-ethylhexyl sebacate droplets. Convective gas mixing was assessed by the aerosol bolus dispersion method. Women with BHR, nonsmokers as well as smokers, showed significantly increased deposition of aerosol particles (nonsmokers: 45.6 +/- 8.8%; smokers: 49.2 +/- 5.4%; mean +/- SD) compared with the control group of female nonsmokers without BHR (38.2 +/- 9.1%; mean +/- SD) (p < 0.01). Aerosol bolus dispersion values showed a trend for higher values in subjects with BHR (nonsmokers: 572 +/- 122 cm3; smokers: 587 +/- 85 cm3) compared with the control group (542 +/- 88 cm3) (p = 0.2). Also, the maximal expiratory flow at 25% vital capacity (MEF25) showed a trend for decreased values in nonsmokers with BHR compared with nonsmokers without BHR (64 +/- 16% of predicted versus 78 +/- 24% of predicted; p = 0.03). These results suggest that deposition of inhaled particles (0.9 micrometer MMAD) administered by the aerosol bolus technique is a sensitive index of peripheral lung injury that is usually not assessable by conventional methods.

Convective gas mixing, airway dimensions and lung function parameters in patients homo- or heterozygote for hereditary α1-antitrypsin deficiency

Informations about convective gas transport and airway morphometry as a function of volumetric lung depth ( V LD) can be evaluated by means of two methods based on aerosol inhalation and determination of aerosol pulse parameters (APP) and effective airway dimensions (EAD). APP, EAD and conventional pulmonary function tests (PFT) were measured in patients homo- and heterozygote for alpha 1-antitrypsin ( α 1-AT) deficiency. Thirteen homozygote subjects (ZZ allele), 21 heterozygote subjects (MZ allele) and 20 healthy controls were included. Anthropometric data were similar in all groups. APP but not PFT and EAD showed slight significant differences between controls and heterozygotes. However, PFT, APP and EAD from ZZ-homozygotes were strongly different from those of the other groups. Differences were also observed for APP between control smokers and nonsmokers and for APP, PFT and EAD between control nonsmokers and heterozygote smokers but not between heterozygote smokers and heterozygote nonsmokers and control nonsmokers and heterozygote nonsmokers, respectively. The data suggest that lung emphysema causes variations of pulmonary convective gas mixing detectable by measurement of APP which obviously precede variations of PFT. Our data further suggest that heterozygotes are not automatically at risk for the development of lung emphysema. Therefore we also regarded the results with request to individual smoking habits and found an increased risk in heterozygote smokers when compared to control nonsmokers.

Aerosol bolus dispersion in healthy subjects.

Aerosol bolus dispersion is a physiological test of lungs, which uses monodisperse submicron particles to measure intrapulmonary convective gas mixing. In this study, aerosol bolus dispersion was measured in healthy subjects in order to assess reference values for possible clinical applications, to assess the reproducibility of these values, and to identify physical and physiological factors influencing aerosol bolus dispersion. Aerosol bolus dispersion was measured in 79 healthy subjects using 20 cm3 aerosol boluses consisting of monodisperse di-2-ethylhexyl sebacate (DEHS) particles. The reproducibility of parameters characterizing the width of the exhaled bolus was of the same order as that of parameters of the flow-volume curve (10%). Aerosol bolus dispersion was independent of the level of lung inflation, and the slope of the relationship between flow rate and dispersion was on average not significantly different from zero (range 100-700 cm3.s-1). Multiple linear regression showed that aerosol bolus dispersion increased with increasing total lung capacity of the subject. We conclude that differences in total lung capacity between individuals should be taken into account when using measures of aerosol bolus dispersion for possible clinical applications.

Thirty month variability of aerosol pulse dispersion and conventional lung function parameters in healthy middle aged smokers and nonsmokers

Chronic cigarette consumption is a generally accepted reason for the development of chronic obstructive pulmonary disease (COPD). COPD correlates to histomorphological parameters of lung structure as well as pulmonary function tests (PFT). COPD related changes affect PFT determined by conventional methods (bodyplethysmography, spirometry) as well as parameters of convective gas mixing. This study evaluates the diagnostic potential of a non-invasive aerosol method for the discrimination between healthy smokers and nonsmokers in comparison to conventional PFT. The aerosol method is based on the inhalation of small aerosol pulses suspended in particle free air and determines their changes during the breathing maneuver. Changes of aerosol pulse parameters (APP) are used to describe the convective component of gas mixing during ventilation. PFT and APP were determined in 40 healthy subjects (nonsmoker: 51.1 ± 1.5 years; smoker: 49.6 ± 1.5 years, 39.1 ± 2.2 pack years) before and after a time interval of 30 months. Conventional PFT in smokers and nonsmokers showed no relevant differences between the values at the beginning and the end of the observation period. Thirty months later, at the end of the observation interval, a very similar behavior of the APP was obtained, which strongly confirmed the prior observed differences between smokers and nonsmokers. The data suggest that cigarette smoke-induced variations of lung function are also detectable in clinically asymptomatic smokers. Even in cases of normal PFT, most APP are able to discriminate between healthy smokers and nonsmokers. Since PFT showed only minor differences between both groups, it is indicated that APP are superior to PFT in the detection of early disturbances of lung ventilation in healthy smokers. Mean values of PFT and APP in smokers and nonsmokers showed a high reproducibility of the data obtained at the beginning of the study as well as at the end of the observation period. The data of our study further confirm that parameters of pulmonary gas exchange and gas mixing are affected by cigarette smoke at an earlier time than parameters of breathing mechanics.

Aerosol bolus dispersion and aerosol-derived airway morphometry: assessment of lung pathology and response to therapy, Part 1.

review discusses the potential utility of two methods using inhaled aerosols to detect and diagnose lung disease and to evaluate the efficacy of therapy. Aerosol bolus dispersion measures convective gas mixing; aerosol-derived airway morphometry assesses the calibers of airway and airspaces. These two methods are discussed in terms of their ease of use (simplicity and acceptability) and current data regarding their validity, reproducibility, specificity, sensitivity, and detection of lung improvement with therapy. Part 1 of this review focuses upon aerosol bolus dispersion; Part 2(1) focuses upon aerosol-derived airway morphometry. Aerosol bolus dispersion has many features that make it clinically attractive. It is simple to administer and patients can successfully perform the maneuvers. It detects known alterations in the lungs. It is reproducible and has high specificity and sensitivity. However, every lung disease or condition known to be detected by aerosol bolus dispersion is also detected by spirometery, maximal expiratory flow-volume curves, or another conventional lung function test. This, aerosol bolus dispersion appears best reserved as a specialized method to supplement conventional lung function tests and to characterize convective gas transport.

Aerosol Bolus Dispersion and Aerosol-Derived Airway Morphometry: Assessment of Lung Pathology and Response to Therapy, Part 2

ABSTRACT This review discusses the potential utility of two methods using inhaled aerosol to detect and diagnose lung disease. Part 1, published earlier,(1) focused upon aerosol bolus dispersion, which measures convective gas mixing. Here, Part 2 focuses upon aerosol-derived airway morphometry (ADAM), which assesses the diameters of airways and acini. This method is discussed in terms of its validity, ability to detect known interventions and diseases, and reproducibility (administering and performing this procedure were already discussed(1). With ADAM, airway and acinar diameters are expressed in terms of the effective airway diameter (EAD), which can be measured as a function of volumetric depth in the lungs. Evidence that ADAM is valid is provided by studies showing EAD agrees well with morphometric indices of airway and acinar size, especially once the distribution of aerosol is accounted for, and changes appropriately in response to known interventions and several diseases. Of particular note is the ...

Convective mixing in human respiratory tract: estimates with aerosol boli.

Convective gas mixing in the respiratory tract of 17 healthy male subjects was studied by an aerosol bolus technique. The monodisperse 1 micron di(2-ethylhexyl)sebacate droplets we used behaved as a nondiffusing gas. As the bolus was inspired to different depths and then expired, we measured the extent to which the bolus spread. We found that the deeper the bolus penetrated into the lungs, the more it became dispersed. The half-width of the expired bolus was a linear function of the volume to which the bolus penetrated at volumetric penetrations of 100-800 cm3. This suggests that convective mixing is not confined to central airways but can also occur in the lung periphery.

Convective gas mixing in the airways of the human lung--comparison of laminar and turbulent dispersion.

A mathematical model of gas transport in the airways of the human lung with numerical solution of the corresponding differential. equation is presented. The model takes into account, along with the summed cross section of. the Weibel lung model, both convection and longitudinal dispersion of helium and sulphur hexafluoride in air. Simulation was performed using two dispersion coefficients corresponding to laminar and disturbed flow. Moreover, since the dispersion coefficients are closely related to the velocity, five constant flow rates were used for each computation and each simulation. Comparison between the model responses to laminar and turbulent dispersion was made in order to determine which plays the preponderant role in gas transport in the human lung. In addition, agreement between the experimental time constant of CO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> elimination during high-frequency ventilation and the predicted mixing time constant was satisfactory. It is concluded that Taylor laminar dispersion cannot play a significant role in the human airways; however, it seems that convective gas mixing with disturbed dispersion-corresponding to a quasi-steady state - can account for most observed gas transport phenomena during spontaneous breathing and high-frequency ventilation.

Pulmonary gas mixing during spontaneous breathing and at high-frequency ventilation

This work is intended to estimate the contribution of either laminar or turbulent dispersion during spontaneous breathing on one hand, and at high-frequency pulmonary ventilation on the other. For that purpose, we performed a computer simulation of a mathematical model of gas transport in the human airways governed by a combination of axial convection and longitudinal dispersion. Calculations were carried out by incorporating two dispersion coefficients, proposed by Taylor and Scherer respectively, into the mathematical model. Moreover, computations were performed with five constant flow rates and two inert heavy (SF 6) and light (He) gases to enhance the effect of mixing. It is concluded that Taylor laminar dispersion cannot play a significant role in the human airways; however, it seems that convective gas mixing with disturbed dispersion - corresponding to a regime of quasi-steady state-can account for most gas transport during spontaneous respiration and high-frequency ventilation.

Convective and diffusive gas mixing in human lungs: experiments and model analysis

Equilibration of inspired with lung residual gas was studied by a single-breath technique for varying breath-holding time with He, Ar, and SF6 as test gases. The ratio of end-expired (FE') to mean lung concentration after expiration (FL) was always below unity, indicating imperfect mixing of gas in the lung. The ratio of FL/FE' for all gases increased with tB, for any tB the ratio was smallest for SF6 and greatest for He. Similarly, Bohr dead space (VD) at any given tB was greatest for SF6 and smallest for He, with VD decreasing toward an asymptotic value common for all gases as tB increased. The results were analyzed quantitatively on a serial three-compartment model of the lung. Model analysis suggests that both diffusion and convection are effective in equilibrating test gases in the lung during breath holding. Further, stratified inhomogeneities in the absence of convective gas mixing in the alveolar space would seriously limit alveolar respiratory gas exchange; with convection, however, stratification is likely to impose only moderate constraints on resting gas exchange.