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1 Experimental Pulmonology Laboratory, Jiménez Díaz Foundation, Autónoma University of Madrid, and 2 Institute of Biofunctional Studies, Complutense University of Madrid, Madrid, Spain. 3 NMR Laboratory, National Centre for Scientific Research and Claude Bernard University, Lyon, France, 4 Red Respira (RTIC C03/11, FIS, ISCIII)
CORRESPONDENCE: G. Peces-Barba, Departamento de Neumología Experimental, Avda Reyes Católicos 2, Fundación Jiménez Díaz, Madrid 28040, Spain. Fax: 34 915504954. E-mail: gpecesba@fjd.es
Keywords: diffusion, experimental animal model, leukocyte elastase, magnetic resonance imaging, pulmonary emphysema
Received: September 11, 2002
Accepted February 14, 2003
This study was supported by the European Community, Brussels, Belgium (V-framework QLG1-2000-01559) and the Ministry of Science and Technology, Madrid, Spain (R+D+I Program in Biomedicine, SAF2000-0115 and P4 Program TIC2000-0376).
| Abstract |
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Nonselective helium-3 gas density coronal ex vivo images and apparent diffusion maps were acquired in control and elastase-induced panacinar emphysema rats. Total lung capacity was considered the reference for both imaging experiments and lung fixation.
A mild degree of emphysema was found based on mean linear intercept (134±25 µm) versus control (85±14 µm). The apparent diffusion coefficients were significantly different between the two groups (0.18±0.02 and 0.15±0.01 cm2·s1 for elastase and control, respectively).
A significant correlation between the apparent diffusion coefficient and corresponding morphometric parameters in mild emphysema was demonstrated for the first time. This study opens the possibility of estimating absolute airspace size using noninvasive techniques.
Early imaging diagnosis of chronic obstructive pulmonary diseases (COPD) is somewhat difficult, despite modern advances in high-resolution thoracic tomography. Human panacinar emphysema is characterised by an increase in lung compliance, a decrease in expiratory flow and some alveolar destruction 1. Elastase induces emphysema in rats with many similarities to human panacinar emphysema, and this has been widely used as a standard animal model for monitoring the initial development of the disease 2, 3. Computed tomography (CT), and particularly thin-section CT, have both become the imaging modalities of choice for assessing the extent and pattern of alveolar destruction 4. As an indirect measurement, CT techniques are of limited sensitivity for depicting changes associated with mild COPD and may even be inaccurate in the presence of pulmonary vascular disease 5. Nuclear medical techniques enable rapid relatively noninvasive physiological assessment of regional ventilation, but the spatial resolution that can be achieved is limited 6. Both CT and nuclear medical techniques expose the patient to ionising radiation and so their use should be limited in longitudinal studies.
Albert et al. 7 recently demonstrated the possibility of magnetic resonance imaging (MRI) of lung tissue filled with the hyperpolarised chemically inert noble gas xenon-129. Since then, the technique has developed, particularly with other noble gas spin nuclei, such as hyperpolarised helium-3, and emerged as a possible alternative to established CT and nuclear medical methods for investigating physiological and physiopathological processes in pulmonary ventilation 6, 8. MRI-based techniques are coming into use in lung research due to their innocuous character and the optimal intrinsic spatial resolution and cross-sectional anatomical visualisation possible 9. They are already being used to provide both static and dynamic ventilation maps of inhaled gases in humans 10, 11 and animals 1214, and to measure gas movement within the spaces of the lung during a respiratory cycle or a breath-hold using diffusion-weighting methods 1517.
The apparent diffusion coefficient (ADC) measured by MRI techniques quantitatively describes the relative ease or difficulty with which a molecule may diffuse within a specific medium (or mobility). This mobility is restricted when molecules are confined in a limited medium by impermeable barriers or hindered by permeable ones, such as alveolar walls. Therefore, the ADC should permit comparison of airway diameters and alveolar sizes, even if the imaging resolution is insufficient to delineate alveolar clusters directly 14.
Emphysema is characterised by significantly enlarged airspaces and destroyed alveolar septa 18, verified and quantified only in terms of post mortem morphometric descriptions such as mean linear intercepts (Lm), mean alveolar internal area (AIA) or destructive index (DI) 19. Additionally, ADC-based MRI techniques are able to detect alveolar enlargements 14, 20, although a direct comparison was not possible due to a difference between fixation volumes and in vivo tidal volumes 14. Moreover, there are some unresolved issues relating to this work, such as the effect of inhaled anaesthesia, 3He/oxygen interactions and the influence of gas exchange on peripheral gas mixing, variables and/or conditions, which, in an initial validation of this technique, can make interpretations difficult. In particular, the influence of 3He/O2 interactions on diffusion-weighted imaging is a very interesting subject that so far has not been sufficiently studied, and requiring additional experiments for quantification of the extent of its effect. This does not invalidate the use of this technique under live conditions, although, in the present study, it was decided to avoid gas mixing by using a simplified post mortem animal model. It might be expected in any case that the estimated ADC increases proportionally with airspace size, forming a noninvasive index of airspace enlargement and possible early emphysema diagnosis. The aim of the present study was to evaluate the potential of ADC-based MRI techniques for estimation of airspace size and diagnosis of mild panacinar emphysema in rats, including interregional correlation with microscopic morphometric results under simplified acceptable experimental conditions.
| Material and methods |
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Magnetic resonance imaging
At 45 days and prior to MRI, the rats were anaesthetised with sodium pentobarbital (60 mg·kg·body weight1 i.p.), tracheotomised and connected to a low-pressure transducer (Honeywell, Morristown, NJ, USA) in order to calculate inspiratory capacity (IC). The IC was obtained by very slow injection of air from the resting volume until an airway pressure of 30 cmH2O was reached. The injection volume was considered to be the IC and the lungs considered to be at total lung capacity. Rats were then sacrificed by inflating the lungs to a pressure of 30 cmH2O with 100% nitrogen and placed in the supine position on a dual-frequency customised radiofrequency coil inside the magnet. Before MRI experiments, rat lungs were kept inflated at IC with nitrogen (N2) in order to avoid atelectases. Before the manoeuvres were started, animals were left for 30 s for lung inflation to reach functional residual capacity and then injected (an IC of 5 mL 3He in N2 per experiment), standardised for equivalent lung capacity conditions to those in morphometric measurements (see below). All MRI experiments were performed within the first hour after sacrificing animals. Reference lung function under the same experimental conditions had already been determined in studies of ventilation distribution in small animals 21. All MRI experiments were performed using a 17-cm diameter bore 2T Oxford magnet (Oxford Instruments, Abingdon, UK) equipped with a Surrey Medical Imaging Systems (Guildford, UK) console. High-density hyperpolarised 3He was obtained by direct optical pumping of a metastable form of 3He, allowing generation of large quantities of polarised gas 22, 23. Polarised 3He was produced at the Laue-Langevin Institute (Grenoble, France) and transported by car to Lyon (France) the day before MRI measurements. Polarisation ranged 1050% (depending on the delay between optical pumping and MRI acquisition).
Ventilation (anatomical) images were obtained using coronal projections with an 8x8-cm square field of view and 256x256 reconstruction matrices acquired using a radial projection reconstruction pulse sequence. For diffusion imaging, this pulse sequence was modified with a pair of nongap diffusion sinusoidal gradients, each of 1 ms duration. Four coronal projections with different diffusion-weighting (the diffusion-weighting factor (b) ranged 028,372 s·cm2) were acquired after gas injection, during breath-hold. ADC maps were obtained from fitting the diffusion-induced signal decay on the four images on a pixel-by-pixel basis. The mean and variance of the ADCs for each animal were calculated by averaging all pixels over the entire pulmonary regions (global intrasubject mean and variance). Unavoidably, these means and variances have contributions from both large and small airways. In order to improve group interregional comparison, three regions were selected with the purpose of excluding large airways as much as possible and then the mean and variance of the ADCs for corresponding pixels in these three different pulmonary regions (mainly upper and lower right lobes and left lung) were also individually determined (regional intrasubject mean and variance) in each animal group. Finally, the mean and variance of the whole set of ADCs for control and emphysematous animals were also calculated by averaging the regional means and variances (regional intersubject means and variances) and the global means and variances (global intersubject means and variances). Additional technical details have previously been reported 24.
Morphometry
After imaging, rat chests were opened and cardiopulmonary blocks removed and fixed by filling with 10% formalin to an airway pressure of 25 cmH2O for 24 h. Sections (5 µm) of each pulmonary region were stained with haematoxylin and eosin. Maps of AIAs as well as horizontal and vertical alveolar lengths, comparable to conventional Lm, were analysed using routine Leica image software (Leica Qwin; Leica Microsystems, Cambridge, UK) on images acquired by means of a video camera (Leica DC 100; Leica Microsystems) adapted to a microscope (Olympus BX40; Olympus, Tokyo, Japan). The software automatically counts intercepts with alveolar walls following a similar scheme to the traditional manual system 25, although it increases the accuracy of the method by computing traces from many more overlaid vertical and horizontal lines.
Statistical analysis
Nonparametric Mann-Whitney U-tests and Wilcoxon signed-rank tests were employed to compare animal groups and pulmonary regions, respectively. Analysis of correlation between MRI and morphometric measurements was performed using the nonparametric Spearman's test. Bland-Altman analysis was finally applied to compare the methods 26. Data are presented as mean±sd.
| Results |
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The IC was measured and shown apparently to have increased (although not significantly) in panacinar (14.7±1.2 mL) versus control (13.3±1.9 mL) animals. Table 1
summarises the data for the three spatially considered ranges (spatial selection based on rat lung structure) and classification of these animals within the experimental intervals of regional intersubject ADC and morphometric results. Owing to the possible influence of the instillation process itself, all of these measurements (MRI-derived and histological) were evaluated for the possible influence of regional distribution, despite the unsatisfactory (although almost inevitable in a reasonable experimental time) dorsolateral projections used, which surely incorporate some data from conducting airways. A first area was selected in the upper right lobe, a second from the distal area of the lower right lobe, and, finally, a third in the medial/distal part of the left lung (fig. 3
). These regions of interest of similar volume were manually outlined with the aid of a computer in the reconstructed ADC maps of both animal groups, and the regional intrasubject ADC data, calculated for each area and animal, were compared to corresponding morphological data obtained in selected fields in the same areas. For morphometry, data (both mean AIA and Lm) were averaged from a minimum of 27±2 microscopic fields located in identical areas to the MRI selected regions. In table 1
, the first range of values was chosen considering only results (ADC and morphometric) from control animals, and then two additional classes were arbitrarily added to categorise animal behaviour versus elastase treatment. The regional intersubject mean ADC (MRI) and alveolar parameters (morphometry) are summarised in table 2
, and reveal a significant difference between the two animal groups (control and elastase rats).
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Direct comparison of regional ADC and morphological data (fig. 4a
) revealed significant linear correlation (Spearman's two-sided correlation coefficient 0.71 for AIA, p<0.001; including data from all animals and from the three selected areas). Similar results were obtained when comparing ADC to Lm (0.70, p<0.001). Additionally, as expected, high correlation between mean AIA and Lm2 (and Lm) was observed (p<0.001, Spearman's two-sided correlation coefficient 0.99). Finally, Bland-Altman concordance analysis was carried out in order to support the previously shown statistical results. Figure 4b
provides information on the absence of evident bias between MRI-derived (ADC) and morphometric measurements (mean alveolar area).
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| Discussion |
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An increase in ADC in emphysematous rats is to be expected because the alveolar dimensions increase with the partial destruction of lung architecture, and, therefore, the gas is subject to less restriction to diffusion. ADC maps in control and emphysematous rats show uniform ADC distribution, probably related to a uniform airspace (enlarged in treated animals). Only evaluation of regional ADCs between the upper and lower portions of the right lobe, and the left lung, revealed significantly higher ADCs in panacinar-like animals with respect to healthy rats. The homogeneous ADC was not surprising, and was consistent with the uniformly altered morphology evident upon morphometric measurements, despite the surely complex regional distribution of elastase solution in the pulmonary airways during the instillation procedure 27.
Taking into account the elastase concentration administered and the calculated Lm (134 µm), the emphysema can be classified as of mild intensity 2. Forty-five days after elastase instillation, lung function and ventilation distribution tests demonstrated significant changes with respect to control animals 3, with minimum inflammatory haemorrhagic component typically present in the first days after instillation. The mean ADC data obtained in the present experiments were very similar to those published previously (0.14 cm2·s1 for control animals and 0.17 cm2·s1 for elastase-treated animals at end-expiratory volume) 14. However, direct comparison with these values is difficult due to significant differences to the present experimental conditions. Thus Lm were higher than those published by the same authors 14, who demonstrated means of 76.5 µm (control) and 97.3 µm (elastase). Among other reasons, these differences could be attributed to the longer study period after elastase instillation in the present case or simply to the different experimental conditions used. Chen et al. 14 could not make a direct comparison between Lm and diffusion coefficient due to a difference between the fixation volumes and the tidal volumes at which MRI experiments were carried out. In the present case, MRI experiments and lung fixation were performed at total lung capacity, which made such comparison possible.
It was hypothesised that this initial stage of the disease is where MRI-based techniques might be very valuable, since CT-based techniques have been shown to be poorly sensitive. Moreover, comparisons 28 or correlations 29, 30 between CT and microscopic morphometry usually fail in mild emphysema. Several morphological criteria have been suggested for the microscopic definition of emphysema, including an increase in AIA, Lm or DI. All of these definitions show poor correlation with macroscopic emphysema evaluation in humans 19, making firm diagnosis of this disease very subjective 31. In addition, correlations between macroscopic emphysema and CT scores also failed in mild emphysema 32. High-resolution CT studies have shown significant correlations with microscopic emphysema parameters 33, but not if only data from subjects with mild emphysema are considered. This technique has not yet been standardised and the imaging quantification of pulmonary emphysema is still not resolved 34.
Experimental settings (for determining morphometric and functional data) in panacinar emphysema have been well-documented and classified 2, 3. The present model facilitates direct comparison between morphometry and airspace MRI with well-preserved ventilation distribution homogeneity in the lung periphery 2, 3. Moreover, the present authors' studies have been performed on dead animals in order to minimise the effect of 3He/O2 interactions and the influence of gas exchange on peripheral gas mixing 21, 35. These two conditions avoid possible artefacts and misinterpretation of MRI diffusion-weighting methods. In addition to this, all manoeuvres started from the same pre-inspiratory lung volume, identical inspiratory volume and equal volume history in order to maintain the same ventilation distribution conditions.
Anatomical (ventilation or gas distribution images) coronal projections were, in general, not very demonstrative of emphysematous disease in the present study. It is well known that the panacinar elastase rat model induces regular distribution of airspace enlargement. Generally speaking, the present images were very similar and fairly uniform, as reported previously by other authors 13, although some minor or subtle ventilation inhomogeneities can be appreciated in some cases (fig. 1
). This result strengthens the conclusion of these same authors, who pointed out that 3He gas density or helium anatomical imaging, at its present level of technical development, is only sensitive to the density of the inhaled gas within the lung and may not be an optimal method for the detection of early-stage emphysema. Nevertheless, much more investigation and further results, particularly those derived from less homogeneous emphysema ventilation patterns that are closer to human characteristics than the elastase model, should provide additional data on lung structure. Additionally, signal attenuation due to diffusion is prohibitively high in this type of imaging (diffusion attenuation factor 0.98 for a 2,000-µs selective pulse and 5-mm slice, reduced to 0.67 for a 1-mm slice and identical parameters; additional signal attenuation is derived from losses in a time constant describing loss in the net magnetisation vector in the transverse plane due to dephasing from spin/spin interactions, diffusion, magnetic field inhomogeneities and other elements (T2*) due to the consequent longer echo times) with small animals, when the strong gradients needed for slice selection and small fields of view are used. For this reason, in micro-imaging applications, only projections (no slice-selection gradient) or thicker slices are currently acquired (e.g. 5-mm slice thickness in 13), which leads to superposition of parenchyma, reductions in the final resolution and complex data interpretation. Future extensions of these studies include time courses following the progression of ADC in this and other animal models. It will equally be very interesting to study other animals with different panacinar and centriacinar emphysema patterns, which may be the basis for future clinical studies with smoking populations, perhaps with incipient emphysema, although with normal lung function and imaging results.
In summary, for the first time, satisfactory correlation between apparent diffusion coefficients obtained by helium-3 diffusion magnetic resonance imaging and the corresponding morphometric data have been demonstrated in three regions of rat lung with mild emphysema. To the best of the present authors' knowledge, this is one of the most favourable morphometry/imaging correlations in mild emphysema. These measurements may be important as a calibration standard for the absolute determination of airspace size via apparent diffusion coefficient measurement.
| Acknowledgements |
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