REVIEW Clinical measurement of end-expiratory lung volume on the intensive care unit nd-expiratory lung volume (EELV) is the volume of gas remaining in the lungs at the end of a normal expiration. It represents the relaxation volume when the recoil pressure of the lung is opposite and equal to the chest wall recoil pressure. (End-expiratory lung volume and functional residual capacity (FRC) are definitions of the same subdivision of lung volume.) EELV measurement is important in the management of patients requiring mechanical ventilation for acute lung injury (ALI) and acute respiratory distress syndrome (ARDS).1 The normal EELV of about 3–4 litres is reduced in ARDS to less than 1 litre2 and in ALI to 1.5 litres.3 In contrast, patients with chronic obstructive pulmonary disease (COPD) often have an increased EELV.4 Furthermore, ventilator setting can increase EELV by application of external positive end-expiratory pressure (PEEP).5 PEEP improves arterial oxygenation by alveolar recruitment and is thereby associated with an increase in EELV. Therefore, the use of PEEP is considered part of the standard therapy for patients with ALI requiring mechanical ventilation.6 Additionally, intrinsic PEEP using inverse ratio ventilation increases EELV.7 Therefore, the ability to assess and monitor EELV accurately is essential in the management of patients requiring mechanical ventilation. The results assist in diagnosis, optimise mechanical ventilatory support, and predict the likelihood of weaning success from the respirator.8 Therefore, several authors have proposed the monitoring of EELV as a tool during mechanical ventilation.8–10 In 1995 the American Thoracic Society and the European Respiratory Society published a workshop report on reference values for EELV.11 This review describes different techniques for EELV measurement, including advantages, disadvantages and possible bed-side use of these techniques on the intensive care unit (ICU). Recently it became obvious that recruitment of lung volume is a phenomenon that occurs in different regions of the lungs.9,12,13 Therefore, a special focus of this review is on those techniques that take into account regional measurements. E normal inspiration and expiration. In adults it is about 700 ml (10 ml/kg). Expiratory reserve volume (ERV) is the gas volume additionally exhaled during forced expiration and inspiratory reserve volume (IRV) is that after a forced inspiration. The sum of VT and IRV is the inspiratory capacity (IC). Even after a maximum expiratory effort, some air is left in the lung; no lung region normally collapses. This persisting gas volume is called residual volume (RV) and amounts to 2–2.5 litres in adults. Expiration stops at residual volume for two reasons: distal airways of diameter ≤2 mm will close before the alveoli collapse;14 the chest wall, rib cage and diaphragm cannot be distorted to the point where all gas in the lung has been exhaled. The EELV – the gas volume remaining in the lungs after an ordinary expiration – amounts to about 3–4 litres, depending on sex, age, height, and weight.15 The existence of this persisting gas volume prevents collapse of the alveoli and ensures that the variation of gas concentration inside the alveoli is minimised. The gas volume in the lung after a maximum inspiration is called the total lung capacity (TLC). In adults, typically, it is 6–8 litres. The volume expired after a maximal inspiration is called the vital capacity (VC) and is therefore equal to the difference between TLC and RV. J Hinz MD, Department of Anaesthesiology, Emergency and Intensive Care Medicine, Georg-August-University, Göttingen, Germany Figure 1. Definitions of lung volumes in normal breathing and during specific TECHNIQUES OF MEASURING LUNG VOLUME manoeuvres such as forced inspiration The different lung volumes, including the EELV, can be estimated by various methods: spirome- IRV and forced expiration. For abbreviations see text. Forced inspiration IC VC TLC VT ERV DEFINITION OF LUNG VOLUMES The gas volume inside the lung is considered in different subdivisions. The definitions of lung volumes in normal breathing and during specific manoeuvres, such as forced inspiration and forced expiration, are shown in Figure 1. Tidal volume (VT) is the gas volume during Normal breathing RV EELV (FRC) Forced expiration ➥ INTERNATIONAL JOURNAL OF INTENSIVE CARE SUMMER 2003 57 Clinical measurement of end-expiratory lung volume try and radiographic techniques (i.e. chest radiographs or computed tomography of the thorax); gas dilution techniques; body plethysmography; respiratory inductive plethysmography; and electrical impedance tomography. The requirements of a technique for lung volume measurement on the ICU are: user-friendly equipment, accuracy of the technique, no radiation exposure to the patient and the capacity for bedside use. Spirometry Spirometry, introduced by Hutchinson,16 measures lung volume during either normal or forced breathing. The classic water spirometer has been replaced by a ‘dry’ spirometer introduced by Fleisch,17 based on the measurement of gas flow through a pneumotachograph. Gas flow is derived from pressure drop over a fixed resistance, which consists of a bundle of parallel capillary tubes or a metal screen. Following the HagenPoiseuille’s-law flow, it is proportional to the pressure drop over the resistance. Volumes are calculated by flow integration over time. Spirometers should be designed to meet the European Thoracic Societies accepted standards.15 Spirometry is the standard method for measuring VT and VC at the bed-side. However, measurement of RV, TLC and EELV, which are not exhaled, is not possible by spirometry. Thus, a different approach to measurement is required for these quantities. Furthermore, the expiratory phase of a spirometry measurement is used to measure obstruction within the lungs. The problem of this method in the intensive care environment is that it requires a co-operative and motivated patient for accurate results. Such conditions, especially in mechanically ventilated patients, are unlikely to be met in the ICU. Body plethysmography Lung volume is measured by the application of Boyle’s law, which states that, under isothermal conditions, when gas in a closed container is compressed, its volume decreases, while the pressure inside the container increases. Therefore the product of volume and pressure, at any given moment, is constant. There are two types of body plethysmographs: variable volume and constant volume. In the variable volume plethysmograph, a change in lung volume is measured direct by a spirometer or pneumotachograph.18 In the constant body plethysmograph, a change in lung volume is measured as a change in box pressure. For the measurement procedure, the patient sits inside an airtight chamber equipped to measure pressure, gas flow, or volume changes, and inhales or exhales to a particular volume (usually end-expiratory lung volume). After a shutter drops across the breathing tube, the patient makes respiratory efforts against the closed shutter, causing the chest volume to expand and decompressing the air in the lungs. The increase in the chest volume slightly reduces the box vol- ume and thus slightly increases the pressure in the box. The most common measurements taken using the body plethysmograph are thoracic gas volume and airway resistance. The advantages of plethysmography are that recording of lung volume takes only a few breaths and can be repeated very quickly between each measurement. The technique shows a high degree of precision indicated by a coefficient of variation of about 5% during repeated measurements.19 The disadvantages of this technique are that the equipment is expensive and requires careful maintenance. Note also that body plethysmography measures the total lung volume including that volume trapped behind closed airways. Therefore, it may deliver different lung volume results compared with data from other measurement techniques. This technique is practicable in spontaneously breathing, co-operative and motivated patients. Although it has been effective in anaesthetised patients, using a specially designed body plethysmograph that allows the patient to be in a supine position,20,21 it is difficult to use with critically ill patients in the intensive care setting and impossible in mechanically ventilated patients. Up to now, no commercially produced body plethysmograph is available for measurement in the supine position. Gas dilution techniques Any gas that is nontoxic and poorly soluble in blood and tissue (e.g. helium, xenon, sulphur hexafluoride (SF6), nitrogen) can be used as tracer gas for measurement of EELV. This technique is either based on rebreathing the tracer gas in a closed circuit, or the wash-in/wash-out of the tracer gas is analysed in a multiple breath procedure. Additionally, information about regional lung volumes and regional ventilation can be derived from mathematical compartmental analysis of tracer wash-out curves.22 A major criticism of this approach to assessment of regional ventilation is that the measurement is not direct and the calculation of regional ventilation depends on assumptions about ideal tracer washout curves. Nitrogen is most frequently used as the tracer gas in multiple breath wash-out investigations. An open circuit multibreath nitrogen wash-out manoeuvre was first described by Darling et al.23 and modified later.24,25 The multiple breath nitrogen wash-out technique measures EELV with a high level of accuracy.24 The necessary change in nitrogen concentration during the wash-in/washout means that oxygen fraction is altered, so that the patient cannot be continuously ventilated with the preselected inspired oxygen fraction. This is a limitation in severe hypoxaemia. The tracer gas sulphur hexafluoride (SF6) provides a solution to this problem by allowing EELV measurements to be taken without interference with the inspired oxygen fraction.26,27 To overcome the problem of wash-in/wash-out ➥ INTERNATIONAL JOURNAL OF 58 SUMMER 2003 INTENSIVE CARE Clinical measurement of end-expiratory lung volume tracer gas techniques needing a fast and sensitive gas analyser to allow breath-by-breath measurements of tracer gas, a technique has been proposed that requires only those analysers frequently used in an ICU. Presuming that air consists mainly of nitrogen, oxygen and carbon dioxide, the tracer gas nitrogen is calculated by deduction from the measurements of oxygen and carbon dioxide concentrations.28 An alternative proposal is a system that collects the expired gas over a number of breaths in a large bag or spirometer and records the mixed expired gas concentration together with expired volume. This solution requires bulky equipment and is difficult in the ICU. A simple helium dilution technique, which utilises a short period of rebreathing six breaths from a 1-litre bag, produces consistent estimations of EELV in those patients suffering from ALI. Xenon has anaesthetic properties, which limit its use in awake patients. During mechanical ventilation, xenon can be used as an interesting research tool.29 When combined with a computed tomogram (CT) study it allows the calculation of both total and regional lung volume.30 Rebreathing techniques require a gas-tight circuit system including the ventilator in order to reach an equilibrium of the tracer gas concentration.31–33 This may be hard to achieve in intubated patients. Wash-in/wash-out procedures are less demanding in this respect, but require as much equipment and effort as rebreathing techniques.34 Gas dilution techniques, whether based on rebreathing or wash-in/wash-out, have the inherent limitation that they can only measure the lung volume that participates in ventilation. Completely closed lung regions behind collapsed airways or mucus plugs will not be detected. Poorly ventilated regions with very long wash-in/wash-out times may also be disregarded. However, ALI appears to be associated more with lung collapse and no ventilation at all than with obstructed airways causing poor ven- Figure 2. The principle of electrical impedance tomography: for electrical impedance measurement an alternating current (5 mA p-p, 50 kHz) is injected between one pair of adjacent electrodes. The resulting surface voltages were measured between the remaining adjacent electrode pairs. All 16 adjacent electrode pairs were used, one pair after the other, as injecting electrodes with the voltages measured with the remaining electrodes. One electrical impedance measurement is completed when all pairs of adjacent electrodes had been used once as injecting electrodes. ~ I Ventral 16 1 2 3 15 14 4 Right 13 5 6 7 11 10 9 Dorsal 8 Chest radiography and computed tomogram Chest radiography shows frontal and lateral views of the lungs. It gives qualitative information about aeration, in case of atelectasis or hyperinflation, but does not allow any quantitative analysis of the EELV. With repeated transverse CT or spiral CT of the chest, EELV can be quantified from a three-dimensional reconstruction of CT slices. This method enables total and regional volume calculation.38,39 Furthermore, information on alveolar recruitment can be obtained from CT scanning.9,40 Unfortunately, CT is not a bedside method and it is associated with radiation exposure. Respiratory inductive plethysmography Respiratory inductive plethysmography (RIP) measures chest and abdomen movement (Respitrace Plus, NIMS Inc., Miami, USA).41,42 It consists of a pair of insulated coils strapped over the upper abdomen and chest. The change of cross-sectional area of the coil caused by chest and abdominal wall displacement modifies the inductance of the coils proportional to tidal volume and lung volume. For calibration of RIP, a simultaneous recording of lung volume by spirometry is necessary. The calibration should be repeated every time that body posture is even slightly changed. RIP is a non-invasive technique which can be used at the bedside on the ICU in mechanically ventilated patients. Unfortunately, Neumann et al.44 found a high and unstable baseline drift of 25.4–29.1 ml/min of the RIP signal from the Respitrace Plus monitor. Although other authors found lower baseline drifts of 1 ml/min,43 they concluded that these high drifts raise doubts about this method, especially for long-term measurements. They found that RIP failed to be consistently accurate enough for quantitative measurement of tidal volume and the determination of EELV.44 Improvement in calibration and long-term stability in RIP may in due course result from a 2002 study by Millard, who introduced more advanced mathematical algorithms to improve the RIP signals.45 Electrical impedance tomography Left U 12 tilation of lung regions.35 Thus, gas dilution techniques may be reasonably accurate for assessing EELV in patients with ALI.24,36,37 Unfortunately, no commercial gas dilution techniques are available for bedside measurement on the ICU. Barber and Brown developed electrical impedance tomography (EIT) in 1984.46 EIT offers the possibility of non-invasive, bedside measurement of EELV, regional lung volume and regional ventilation.47–50 The principle of EIT is based on a small alternate current injection (5 mA, pp) and voltage measurement via surface electrodes placed around the thorax (Figure 2). The electrical properties of the chest vary depending on changes in the air content. Therefore, chan- ➥ INTERNATIONAL JOURNAL OF 60 SUMMER 2003 INTENSIVE CARE Clinical measurement of end-expiratory lung volume routine usage it should be simple and not susceptible to disturbances. The technique should measure the EELV accurately and thereby offer a rational basis for therapeutic consequences. The patient should not be endangered by an invasive method or radiation exposure. To avoid the risk in volved in transport of the patient to the measurement device, the capacity for bedside use is important. Therefore, the technique should be brought to the patient and not the patient to the technique. Any sudden change of lung volume, whether due to change of respirator setting or the progress of lung injury, should be detected immediately: therefore a continuous measurement of EELV is desirable. Additionally, to recognise heterogeneity in regional lung volume and regional ventilation a technique is desirable which delivers information about regional lung volume and regional ventilation. As yet no technique exists that fully complies with all these demands. Tables 1–3 give detailed information about advantages and disadvantages, possible bedside use and the ability to obtain regional parameters from the different techniques for lung volume measurement. From the above, only electrical impedance tomography gets close to complying with all demands. During the next few years, electrical impedance tomography has to prove if it can become a routine tool for the measurement of EELV, regional lung volume and regional ventilation on the ICU. (EELV) measurement by electrical impedance tomography during mechanical ventilation with identical tidal volume at CONCLUSION different positive end-expiratory pres- Bedside measurement of EELV is desirable, but not yet standard practice on the ICU. The unfulfilled need for a simple and preferably automated technique has so far limited the acceptance of measuring EELV in the intensive care setting. Electrical impedance tomography may become a simple bedside method for monitoring change in EELV in the near future. 0.20 DISCUSSION EELV 1,285 mL EELV 1,610 mL EELV 1,885 mL sures (PEEP 0, PEEP 5, PEEP 10, and PEEP 15) in one patient. The figure shows four examples of lung impedance time course (∆impedance) at different lung volumes induced by different PEEP. Note that the end-expiratory lung impedance (ELI) increased with increasing EELV. EELV 2,211 mL 0.15 ∆ Impedance It may appear surprising that so many techniques, even some that can be used at the bedside, have been refined for EELV measurement in mechanically ventilated patients, yet the use of EELV as a guide in the treatment of the patient and setting of the ventilator is still not common in the ICU. The reasons seem to be that the process of measurement is complicated and the benefit is not perceived not warrant the effort. The lack of access to a simple, and preferably automated, technique has so far limited the use of EELV measurement as accepted practice in intensive care. The requirements for an appropriate technique for lung volume measurement on the ICU are manifold. In a time of straitened financial resources the technique used should be cheap. For Figure 3. End-expiratory lung volume Tidal volume ges in lung impedance induced by changes in lung volume can be reconstructed.47 EIT was validated by comparison of regional aeration at different tidal volumes and lung volumes derived from computed tomography.51 The study confirmed that EIT is a suitable, non-invasive method for detecting regional changes in lung volume and monitoring local effects of artificial ventilation. EIT was compared to ventilation scintigraphy in mechanically ventilated pigs,52 and the authors concluded that it seems to allow real time monitoring of regional ventilation distribution at the bedside. The major advantages of EIT are that it is non-invasive, easy to use at the bedside and that data collection can be performed with a high time and local resolution. According to Hahn et al., the minimal detectable regional lung volume by EIT is in the range of 9–29 ml.53 Barber and Brown54 found a spatial resolution of approximately 8% of the thorax diameter, so that within the thorax a resolution of 8 ml is achieved. A study performed by Hinz et al. showed that a PEEP-induced increase of EELV is accompanied by a proportional increase of end-expiratory lung impedance (ELI).3 An example of end-expiratory lung impedance at different measurements of EELV is shown in Figure 3. However, use of ELI results in a slight underestimate of lung volume changes. The reasons are, first, that impedance changes within the lung are generated either by the air content or changes of the central blood volume by the pulsatile blood flow;55 second, that pulmonary air content and impedance change may not correlate linearly, if stretching of lung parenchyma itself causes impedance changes; and, third, that impedance is linearly correlated to the impedance of a polyacrylamide gel, up to an increase of 20%.56 If gels with higher impedance were used, the changes were underestimated by the EIT system. This result may depend either on the electrical properties of the EIT system57 used or on the image reconstruction algorithm.58 0.10 ELI PEEP 15 0.05 0.00 ELI PEEP 10 -0.05 ELI PEEP 0 ELI PEEP 5 Time (not scaled) ➥ INTERNATIONAL JOURNAL OF INTENSIVE CARE SUMMER 2003 61 Clinical measurement of end-expiratory lung volume Table 1. Methods for measuring lung volumes, their principles, advantages and disadvantages. The ability to measure regional lung volume and regional ventilation (regional parameter) and the possibility of bedside use on the ICU are noted Method Principle Advantage/disadvantage Regional parameter Bed-side Spirometry Classic water spirometer has been replaced by ‘dry’ It measures tidal volume and vital capacity. It needs a spirometer based on the technique of pneumotachography. co-operative and motivated subject, so is unlikely to be Application of Hagen-Poiseuille’s law appropriate in the ICU, especially in mechanically ventilated patients Body plethysmography Application of Boyle’s law: patient in closed box, panting against an occluded shutter with the recording of airway and box pressures Reference technique. Requires expensive equipment. Measures all gases in the lung even behind occluded airways and gas in poorly ventilated regions. Enables measurement in rapid sequence Respiratory inductive plethysmography (RIP) RIP measures chest and abdomen movement by a pair of insulated coils strapped over the upper abdomen and chest. This displacement modifies the inductance of the coils proportional to tidal volume and lung volume High and unstable signal baseline drift ✔ ✔ Table 2. Wash-in/wash-out techniques of measuring lung volumes, their principles, advantages and disadvantages. The ability to measure regional lung volume and regional ventilation (regional parameter) and the possibility of bedside use on the ICU are noted Method Principle Advantage/disadvantage Regional parameter Bed-side Helium rebreathing Rebreathing of the poorly soluble helium until full mixing between lung volume and spirometer Requires CO2 absorber in circuit and O2 to compensate for the uptake ✔ Multiple breath N2 wash-out Wash-out of N2 in lung by O2 breathing. Knowing the initial and final N2 concentrations in lung gas and the expired amount of N2, lung volume can be calculated Less reliable if patient is ventilated with high fractions of O2, because less N2 can be washed out. Some of expired N2 comes from body stores and must be subtracted before the calculation of EELV ✔ Xenon wash-in/ wash-out Wash-in of a tracer gas that does not normally exist in the Xenon attenuates x-rays which may enable regional lungs and then wash-out similar to N2 wash-out volume radiographs; poor resolution, anaesthetic properties ✔ SF6 wash-in/wash-out Wash-in of a tracer gas that does not normally exist in the Very low concentration of tracer gas, which allows lungs and then wash-out similar to N2 wash-out maintenance of inspired oxygen fraction ✔ N2 wash-out An inspired VC of O2, followed by slow expiration to RV during the recording of N2 Easy and rapid to perform. Less accurate than multiple breath wash-out ✔ Helium wash-out Inspired VC of O2 with 5–10% helium, followed by slow expiration to RV during the recording of N2 Less reliable than multiple breath techniques. Can be used with other tracer gases, for example SF6 ✔ Multiple breath methods Single breath methods Table 3. Imaging techniques of measuring lung volumes, their principles, advantages and disadvantages. The ability to measure regional lung volume and regional ventilation (regional parameter) and the possibility of bedside use on the ICU are noted Method Principle Advantage/disadvantage Regional parameter Bed-side Chest radiography Frontal and lateral view of the lungs Gives qualitative information but does not allow any quantitative analysis ✔ Computed tomogram Repeated transverse CT scans or spiral CT of the chest during breath-hold Not a bedside technique. Enables regional volume calculation ✔ Isotope techniques 133X Similar to SF6 wash-in/wash-out Expensive equipment and radiation ✔ Electrical impedance tomography Delivers total and regional lung volumes, and regional ventilation, non-invasive, radiation-free, bedside use, continuous measurement possible ✔ Reconstruction of impedance change via surface electrodes placed around the thorax induced by alternate current injection and voltage measurement ACKNOWLEDGEMENT I would like to thank Onnen Moerer, Department of Anaesthesiology, Emergency and Intensive Care Medicine, GeorgAugust-University, Göttingen, Germany for his valuable cooperation and expert advice. 3. REFERENCES 4. 1. 2. Ashbaugh DG, Bigelow DB, Petty TL et al. Acute respiratory distress in adults. Lancet 1967; 7511: 319–323. Macnaughton PD, Evans TW. Measurement of lung vol- 5. ✔ ✔ ume and DLCO in acute respiratory failure. Am J Respir Crit Care Med 2003; 150: 770–775. Hinz J, Hahn G, Neumann P et al. End-expiratory lung impedance change enables bedside monitoring of endexpiratory lung volume change. Intensive Care Med 2003; 29: 37–43. Spence DP, Kelly YJ, Ahmed J et al. Critical evaluation of computerised x ray planimetry for the measurement of lung volumes. Thorax 1995; 4: 383–386. Bernard GR, Artigas A, Brigham KL et al. Report of the ➥ INTERNATIONAL JOURNAL OF 62 SUMMER 2003 INTENSIVE CARE Clinical measurement of end-expiratory lung volume 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. 16. 17. 18. 19. 20. 21. 22. 23. 24. 25. American-European Consensus conference on acute respiratory distress syndrome: definitions, mechanisms, relevant outcomes, and clinical trial coordination. Consensus Committee. J Crit Care 1994; 1: 72–81. Mancebo J. PEEP, ARDS, and alveolar recruitment. Intensive Care Med 1992; 18: 383–385. Cole A, Weiler S, and Sykes M. Inverse ratio ventilation compared with PEEP in adult respiratory failure. Intensive Care Med 1998; 24: 227–232. Hedenstierna G. The recording of FRC – Is it of importance and can it be made simple? Intensive Care Med 1993; 19: 365–366. Gattinoni L, Pelosi P, Crotti S et al. Effects of positive end-expiratory pressure on regional distribution of tidal volume and recruitment in adult respiratory distress syndrome. Am J Respir Crit Care Med 1995; 6: 1807–1814. Dambrosio M, Roupie E, Mollet JJ et al. Effects of positive end-expiratory pressure and different tidal volumes on alveolar recruitment and hyperinflation. Anesthesiology 1997; 3: 495–503. Stocks J, Quanjer PH. Reference values for residual volume, functional residual capacity and total lung capacity. ATS Workshop on Lung Volume Measurements. Official Statement of The European Respiratory Society. Eur Respir J 1995; 3: 492–506. Pelosi P, Goldner M, McKibben A et al. Recruitment and derecruitment during acute respiratory failure: an experimental study. Am J Respir Crit Care Med 2001; 1: 122–130. Crotti S, Mascheroni D, Caironi P et al. Recruitment and derecruitment during acute respiratory failure: a clinical study. Am J Respir Crit Care Med 2001; 1: 131–140. Leith DE, Mead J. Mechanisms determining residual volume of the lungs in normal subjects. J Appl Physiol 1967; 2: 221–227. Quanjer PH, Tammeling GJ, Cotes JE et al. Lung volumes and forced ventilatory flows. Report Working Party Standardization of Lung Function Tests, European Community for Steel and Coal. Official Statement of the European Respiratory Society. Eur Respir J Suppl 1993; 16: 5–40. Hutchinson J. On the capacity of the lung, and on the respiratory functions, with a view of detecting disease by spirometer. Med Chir Trans 1846; 11: 137–252. Fleisch A. Der Pneumotachograph: ein Apparat zur Geschwindigkeitsregulierung der Atemluft. Plügers Arch ges Physio 1925; 209: 713–722. Mead J, Loring SH. Analysis of volume displacement and length changes of the diaphragm during breathing. J Appl Physiol 1982; 3: 750–755. DuBois AB, Botelho SY, Bedell GN et al. A rapid plethysmographic method for measuring thoracic gas volume: a comparison with a nitrogen wash-out method for measuring functional residual capacity in normal subjects. J Clin Invest 1955; 35: 322–326. Hedenstierna G, Lofstrom B, Lundh R. Thoracic gas volume and chest-abdomen dimensions during anesthesia and muscle paralysis. Anesthesiology 1981; 5: 499–506. Westbrook PR, Stubbs SE, Sessler AD et al. Effects of anesthesia and muscle paralysis on respiratory mechanics in normal man. J Appl Physiol 1973; 1: 81–86. Cumming G and Guyatt AR: Alveolar gas mixing efficiency in the human lung. Clin Sci.(Colch.) 1982; 5: 541–547. Darling RC, Richards DW, Cournant A. Studies on intrapulmonary mixture of gases. Open circuit method for measuring residual air. J Clin Invest 1940; 19: 609–618. Wrigge H, Sydow M, Zinserling J et al. Determination of functional residual capacity (FRC) by multibreath nitrogen washout in a lung model and in mechanically ventilated patients. Accuracy depends on continuous dynamic compensation for changes of gas sampling delay time. Intensive Care Med 1998; 24: 487–493. Cournand A, Yarmouth IG, Riley RL. Influence of body size on gaseous nitrogen elemination during high oxygen breathing. Proc Soc Exp Biol 1941; 48: 280–284. 26. Jonmarker C, Jansson L, Jonson B et al. Measurement of functional residual capacity by sulfur hexafluoride washout. Anesthesiology 1985; 1: 89–95. 27. East TD, Wortelboer PJ, van Ark E et al. Automated sulfur hexafluoride washout functional residual capacity measurement system for any mode of mechanical ventilation as well as spontaneous respiration. Crit Care Med 1990; 1: 84–91. 28. Fretschner R, Deusch H, Weitnauer A et al. A simple method to estimate functional residual capacity in mechanically ventilated patients. Intensive Care Med 1993; 7: 372–376. 29. Tomiyama N, Takeuchi N, Imanaka H et al. Mechanism of gravity-dependent atelectasis. Analysis by nonradioactive xenon-enhanced dynamic computed tomography. Invest Radiol 1993; 7: 633–638. 30. Murphy DM, Nicewicz JT, Zabbatino SM et al. Local pulmonary ventilation using nonradioactive xenon-enhanced ultrafast computed tomography. Chest 1989; 4: 799–804. 31. Suter PM and Schlobohm RM. Determination of functional residual capacity during mechanical ventilation. Anesthesiology 1974; 6: 605–607. 32. Gillespie DJ. Use of an acoustic helium analyzer and microprocessor for rapid measurement of absolute lung volume during mechanical ventilation. Crit Care Med 1985; 2: 118–121. 33. Macnaughton PD, Morgan CJ, Denison DM et al. Measurement of carbon monoxide transfer and lung volume in ventilated subjects. Eur Respir J 1993; 2: 231–236. 34. Black AM, Hahn CE, Maynard P et al. Measurement of lung volume by multiple indicator dilution. Differences in apparent volumes of distribution of oxygen, nitrogen and argon. Br J Anaesth 1984; 3: 289–298. 35. Dantzker DR, Brook CJ, Dehart P et al. Ventilation-perfusion distributions in the adult respiratory distress syndrome. Am Rev Respir Dis 1979; 5: 1039–1052. 36. Ibanez J, Raurich JM, Moris SG. Measurement of functional residual capacity during mechanical ventilation. Comparison of a computerized open nitrogen washout method with a closed helium dilution method. Intensive Care Med 1983; 9: 91–93. 37. Mitchell RR, Wilson RM, Holzapfel L et al. Oxygen washin method for monitoring functional residual capacity. Crit Care Med 1982; 8: 529–533. 38. Rosenblum LJ, Mauceri RA, Wellenstein DE et al. Density patterns in the normal lung as determined by computed tomography. Radiology 1980; 2: 409–416. 39. Rosenblum LJ, Mauceri RA, Wellenstein DE et al. Computed tomography of the lung. Radiology 1978; 2: 521–524. 40. Gattinoni L, Presenti A, Torresin A et al. Adult respiratory distress syndrome profiles by computed tomography. J Thorac Imaging 1986; 1: 25–30. 41. Abraham WM, Watson H, Schneider A et al. Noninvasive ventilatory monitoring by respiratory inductive plethysmography in conscious sheep. J Appl Physiol 1981; 6: 1657–1661. 42. Milledge JS and Stott FD: Inductive plethysmography – a new respiratory transducer. J Physiol 1977; 1: 4P–5P. 43. Valta P, Takala J, Foster R et al. Evaluation of respiratory inductive plethysmography in the measurement of breathing pattern and PEEP-induced changes in lung volume. Chest 1992; 1: 234–238. 44. Neumann P, Zinserling J, Haase C et al. Evaluation of respiratory inductive plethysmography in controlled ventilation: measurement of tidal volume and PEEP-induced changes of end-expiratory lung volume. Chest 1998; 2: 443–451. 45. Millard RK. Key to better qualitative diagnostic calibrations in respiratory inductive plethysmography. Physiol Meas 2002; 2: N1–N8. 46. Barber DC, Brown BH. Applied potential tomography. J Phys E Sci Instrum 1984; 17: 723–733. 47. Frerichs I. Electrical impedance tomography (EIT) in applications related to lung and ventilation: a review of ➥ INTERNATIONAL JOURNAL OF 64 SUMMER 2003 INTENSIVE CARE Clinical measurement of end-expiratory lung volume 48. 49. 50. 51. 52. 53. 54. experimental and clinical activities. Physiol Meas 2000; 2: R1–21. Hahn G, Sipinkova I, Baisch F et al. Changes in the thoracic impedance distribution under different ventilatory conditions. Physiol Meas 1995; 3(Suppl A): A161–A173. Adler A, Amyot R, Guardo R et al. Monitoring changes in lung air and liquid volumes with electrical impedance tomography. J Appl Physiol 1997; 5: 1762–1767. Adler A, Shinozuka N, Berthiaume Y et al. Electrical impedance tomography can monitor dynamic hyperinflation in dogs. J Appl Physiol 1998; 2: 726–732. Frerichs I, Hinz J, Herrmann P et al. Detection of local lung air content by electrical impedance tomography compared with electron beam CT. J Appl Physiol 2002; 2: 660–666. Hinz J, Neumann P, Dudykevych T et al. Regional ventilation by Electrical Impedance Tomography – A comparison with ventilation scintigraphy in pigs. Chest 2003; in press. Hahn G, Hartung C, Hellige G. Bestimmung der Grösse minimal erfassbarer Areale mit Ventilationsstörungen. Gustav Fischer Verlag, Mainz 1998 Funktionsanalyse biologischer Systeme; 6.2.5: 77–77. Brown BH, Barber DC. Electrical impedance tomography; the construction and application to physiological measurement of electrical impedance images. Med Prog Technol 1987; 2: 69–75. 55. Faes TJ, van der Meij HA, de Munck JC et al. The electric resistivity of human tissues (100 Hz–10 MHz): a metaanalysis of review studies. Physiol Meas 1999; 4: R1–10. 56. Holder DS, Khan A. Use of polyacrylamide gels in a saline-filled tank to determine the linearity of the Sheffield Mark 1 electrical impedance tomography (EIT) system in measuring impedance disturbances. Physiol Meas 1994; 15(Suppl 2a): A45–A50. 57. Brown BH, Seagar AD. The Sheffield data collection system. Clin Phys Physiol Meas 1987; 8: 91–97. 58. Barber DC. Quantification in impedance imaging. Clin Phys Physiol Meas 1990; 11(Suppl A): 45–56. ■ Correspondence to: José Hinz MD Department of Anaesthesiology, Emergency and Intensive Care Medicine Georg-August-University Robert-Koch-Str. 40 D-37075 Göttingen, Germany e-mail: [email protected] INTERNATIONAL JOURNAL OF INTENSIVE CARE SUMMER 2003 65
© Copyright 2026 Paperzz