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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Journal of clinical monitoring and computing 12 (1996), S. 231-236 
    ISSN: 1573-2614
    Keywords: Pulmonary carbon dioxide elimination ; tissue carbon dioxide production ; capnography ; end-tidal PCO2 ; dead space
    Source: Springer Online Journal Archives 1860-2000
    Topics: Computer Science , Medicine
    Notes: Abstract Objective. The pulmonary elimination of the volume of CO2 per breath (VCO2/br, integration of product of airway flow ( $$\dot V$$ ) and PCO2 over a single breath) is a sensitive monitor of cardio-pulmonary function and tissue metabolism. Negligible inspired PCO2 results when the capnometry sampling site (SS) is positioned at the entry of the inspiratory limb to the airway circuit. In this study, we test the hypothesis that moving SS lungward will result in significant inspired CO2 (VCO2[I]), that needs to be excluded from VCO2/br.Methods. We ventilated a mechanical lung simulator with tidal volume (VT) of 800 mL at 10 breaths/min. CO2 production, generated by burning butane in a separate chamber, was delivered to the lung. Airway $$\dot V$$ and PCO2 were measured (Capnomac Ultima, Datex), digitized (100 Hz for 60 s), and stored by microcomputer. Then, computer algorithms corrected for phase diferences between $$\dot V$$ and PCO2 and calculated expired and inspired VCO2 (VCO2[E] and VCO2[I]) for each breath, whose difference equalled overall VCO2/br. The lung and Y-adapter (where the inspiratory and expiratory limbs of the circuit joined) were connected by the SS and a connecting tube in varying order.Results. During ventilation of the lung model (VT = 800 ml) with SS adjacent to the inspiratory limb, VCO2[E] was 16.8± 0.4 ml and VCO2[I] was 1.1 ±0.1 ml, resulting in overall VCO2/br (VCO2[E] —VCO2[I]) of 15.7 ± 0.4 ml. If VCO2[I] was ignored in the determination of VCO2/br, then the %error that VCO2[E] overestimated VCO2/br was 7.2± 0.3%. This %error significantly increased (p 〈 0.05, Student's t-test) when VT was decreased to 500 mL (%error = 12.4 ± 0.8%) or when SS was moved to the lungward side of a 60 mL connecting tube (VCO2[I] = 2.8 ± 0.2, %error = 18.2 ± 1.6) or a 140 mL tube (VCO2[I] = 5.9±03 mL, %error = 37.5±3.3).Conclusions. When the SS was moved lungward from the inspiratory limb, instrumental dead space (VD INSTR) increased and, at end-expiration, contained exhaled CO2 from the previous breath. During the next inspiration, this CO2 was rebreathed relative to SS (i.e. VCO2[I]), and contributed to VCO2[E]. Thus, VCO2[E] overestimated VCO2/br (%error) by the amount of rebreathing, which was exacerbated by largerVD INSTR (increased VCO2[I]) or smaller VT (increased VCO2[I]-to-VCO2/br ratio).
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Journal of clinical monitoring and computing 14 (1998), S. 265-270 
    ISSN: 1573-2614
    Keywords: Pulmonary CO2 elimination ; CO2 expirogram ; mechanical lung model ; sequential expiration ; alcohol-burning metabolic chamber ; gas trapping ; oximetry
    Source: Springer Online Journal Archives 1860-2000
    Topics: Computer Science , Medicine
    Notes: Abstract Objective. We have previously shown in a mechanical lung model [1] that bronchial flap-valve expiratory obstruction results in sequential lung expiration, best detected by prolonged and low magnitude tracheal expired flow ( $${{\dot V}}$$ ) from the obstructed lung. However, the normal expiratory resistance of clinical ventilation circuits might also generate prolonged, low value exhaled $${{\dot V}}$$ , that could be confused with bronchial flap-valve obstruction. We reasoned that bronchial flap-valve obstruction would also cause sequential CO2 unloading from each lung and result in a biphasic tracheal capnogram. Methods. To test this hypothesis, we ventilated (VT, 650 ml; f, 10 br/min) a dual mechanical test lung, with each side connected to a separate alcohol-burning chamber. An airway adapter-monitor system measured airway $${{\dot V}}$$ , P, PCO2, and FO2. The circumference of the diaphragm in a respiratory one-way valve was trimmed to generate unidirectional resistance to expiratory $${{\dot V}}$$ . Measurement sequences were repeated after this flap-valve was interposed in the left “main-stem bronchus.” Results and Discussion. During moderate or severe left bronchial flap-valve obstruction, left bronchial $${{\dot V}}$$ was delayed so that the left lung anatomical dead space (devoid of CO2) mixed with normal right exhalate to depress the expiratory upstroke or early plateau of the tracheal capnogram. During severe obstruction, decreased perfusion of the left lung caused lower alveolar PCO2. Then, prolonged low $${{\dot V}}$$ from the left bronchus also resulted in depression of the end of the tracheal alveolar plateau. In general, the low magnitude of bronchial $${{\dot V}}$$ from the obstructed lung limited its effect on the tracheal capnogram and the best marker of sequential lung emptying during bronchial flap-valve obstruction may be late exhaled $${{\dot V}}$$ without reduction in total tidal volume.
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Journal of clinical monitoring and computing 16 (2000), S. 351-360 
    ISSN: 1573-2614
    Keywords: carbon dioxide ; oxygen ; kinetics ; non-steady state ; cardiac output ; PEEP ; pulmonary embolism ; pulmonary gas exchange monitoring
    Source: Springer Online Journal Archives 1860-2000
    Topics: Computer Science , Medicine
    Notes: Abstract Traditionally, the study of CO2 and O2 kinetics in the body has been mostly confined to equilibrium conditions. However, the peri-anesthesia period and the critical care arena often involve conditions of non-steady state. The detection and explanation of CO2 kinetics during non-steady state pathophysiology have required the development of new methodologies, including the CO2 expirogram, average alveolar expired PCO2, and CO2 volume exhaled per breath. Several clinically relevant examples of non-steady state CO2 kinetics perturbations are examined, including abrupt decrease in cardiac output, application of positive end-expiratory pressure during mechanical ventilation, and occurrence of pulmonary embolism. The lesser known area of non-steady state O2 kinetics is introduced, including the measurement of pulmonary O2 uptake per breath. Future directions include the study of the respiratory quotient per breath, where the anaerobic threshold during anesthesia is identified by increasing respiratory quotient.
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    Annals of biomedical engineering 28 (2000), S. 1159-1164 
    ISSN: 1573-9686
    Keywords: Oxygen consumption ; ATPS ; STPD ; Tissue metabolism
    Source: Springer Online Journal Archives 1860-2000
    Topics: Medicine , Technology
    Notes: Abstract Traditionally, measurement of pulmonary O2 uptake uses mass balance of N2 to correct for differences between inspired and expired volume (V) due to temperature (T) and relative humidity (RH). Often during anesthesia, N2 balance cannot be invoked due to high inspired O2 fraction (FIO2) or nonsteady state conditions. Then, O2 uptake per breath (VO2,br) must use assumed or measured T and RH differences between inspirate and expirate. This numerical analysis study examines how errors in inspired RH and T can affect VO2,br. Equations were developed to simulate a baseline metabolic and ventilatory condition. A unit error in inspired RH of 0.5 (during constant inspired T of 22°C) caused percent errors in VO2,br of 5.6% during FIO2 = 0.2% and 28.8% during FIO2 of unity. Percent error in VO2,br was given by (-57.6 FIO2 -0.115) ⋅(change in RH) $$ \left( {R^2 〉0.999} \right) $$ . Errors in inspired T (during constant inspired RH of 0.5) had similar effects on percent error in $$ V_{O_2 ,br} \left( { = - 8.75F_{I_{O_2 } } - 0.093} \right) $$ ⋅(change in T) $$ V_{O_2 ,br} \left( { = - 8.75F_{I_{O_2 } } - 0.093} \right) $$ Because inspired $$ V_{O_2 } $$ is larger at higher $$ F_{I_{O_2 } } $$ and because $$ V_{O_2 ,br} $$ is the difference between inspired and expired $$ V_{O_2 } $$ $$ V_{O_2 ,br} $$ is most affected by the inspired V error at the largest $$F_{I_{O_2 } } $$ When tissue O2 consumption decreases relative to minute ventilation, T and RH errors have a greater effect on $$ V_{_{O_2 } ,br} $$ because the error in inspired V affects a smaller $$ V_{_{O_2 } ,br} $$ At lower barometric pressure, RH errors affect $$ V_{_{O_2 } ,br} $$ more because water vapor V occupies a larger fraction of inspired V. In summary, because inspired RH and T can vary significantly during anesthesia, a fast-response humidity and T sensor, combined with flow and $$ F_{O_2 } $$ measurements, are needed to allow accurate determination of $$ V_{O_2 ,br} $$ $$ V_{O_2 ,br} $$ should become an important measure of metabolism and patient wellness during anesthesia. © 2000 Biomedical Engineering Society. PAC00: 8719Uv, 8719Pp
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