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Brazilian Journal of Medical and Biological Research

Print version ISSN 0100-879XOn-line version ISSN 1414-431X

Braz J Med Biol Res vol. 31 no. 3 Ribeirão Preto Mar. 1998

http://dx.doi.org/10.1590/S0100-879X1998000300018 

Braz J Med Biol Res, March 1998, Volume 31(3) 445-450

Paraquat poisoning: an experimental model of dose-dependent acute lung injury due to surfactant dysfunction

M.F.R. Silva and P.H.N. Saldiva

Laboratório de Poluição Atmosférica Experimental, Faculdade de Medicina, Universidade de São Paulo, São Paulo, SP, Brasil

Abstract
Introduction
Material and Methods
Results
Discussion
References
Correspondence and Footnotes


Abstract

Since the most characteristic feature of paraquat poisoning is lung damage, a prospective controlled study was performed on excised rat lungs in order to estimate the intensity of lesion after different doses. Twenty-five male, 2-3-month-old non-SPF Wistar rats, divided into 5 groups, received paraquat dichloride in a single intraperitoneal injection (0, 1, 5, 25, or 50 mg/kg body weight) 24 h before the experiment. Static pressure-volume (PV) curves were performed in air- and saline-filled lungs; an estimator of surface tension and tissue works was computed by integrating the area of both curves and reported as work/ml of volume displacement. Paraquat induced a dose-dependent increase of inspiratory surface tension work that reached a significant two-fold order of magnitude for 25 and 50 mg/kg body weight (P<0.05, ANOVA), sparing lung tissue. This kind of lesion was probably due to functional abnormalities of the surfactant system, as was shown by the increase in the hysteresis of the paraquat groups at the highest doses. Hence, paraquat poisoning provides a suitable model of acute lung injury with alveolar instability that can be easily used in experimental protocols of mechanical ventilation.

Key words: paraquat, experimental model, acute lung injury, pressure-volume curve, respiratory work


Introduction

Paraquat, a herbicide widely used in agriculture, has caused many deaths due to suicidal or accidental ingestion. The primary damage in mammals occurs in the lung. The pathogenesis of paraquat-induced damage to alveolar structure is related to its accumulation in type II pneumocytes (1). The concentration of paraquat in the lung after exposure rises progressively to several times that in plasma or in any other organ. Besides pulmonary insufficiency, central nervous derangements and hepatic and renal tubular lesions may also be present, but such toxicity is observed only after intoxication with high doses. The degree of lung damage seems to be dose-dependent (2), is enhanced by high oxygen concentrations (3) and persists in spite of lowering paraquat levels by hemoperfusion (1).

Lung dynamic behavior has different components, and many studies have focused on separating the effects of tissue dissipation and flow through the airway tree on lung resistance, and on the effects of surface tension in elastance (4,5). It is of considerable interest to separate lung injury due to connective tissue alteration (e.g., emphysema) from injury due to an increase in surface tension (e.g., respiratory distress syndrome).

Due to its simplicity (single ip administration), low cost and rapid effect, paraquat intoxication is a suitable model of acute lung injury to be used in protocols of mechanical ventilation. In the present study we focused on the dose-response effect of paraquat to determine whether it is possible to obtain pulmonary lesions of increasing severity, and on separating the participation of tissue and alveolar surface tension in the acute lesion.


Material and Methods

Experimental groups

Paraquat dichloride dissolved in saline solution (0.9% NaCl) was administered in a single intraperitoneal injection to non-SPF Wistar rats weighing 213.62 ± 22.50 g. Doses ranged from zero to 50 mg/kg body weight and the animals were studied 24 h later. Twenty-nine rats were allocated to 5 groups: control (N = 9) and 1 mg/kg, 5 mg/kg, 25 mg/kg and 50 mg/kg body weight of paraquat (5 animals/group).

Lung preparation and apparatus

The animals were anesthetized with pentobarbital sodium (30 mg/kg body weight) and sacrificed by exsanguination via the abdominal aorta. The lungs were surgically exposed and allowed to collapse freely, and removed en bloc. The heart was dissected away. In order to measure the pressure-volume relationship, the lungs were placed in a 280-ml plethysmograph connected to a graded pipette. The tracheal cannula was connected to a 20-ml syringe and to a small vertical column partially filled with water. When lungs were inflated with air from the syringe, the volume was measured by the displacement of a detergent bubble in the pipette (Figure 1). Initially, lungs were subjected to three previous inflations up to 30 cmH2O and then allowed to return to their resting volume. Lungs were filled with air in small increments of volume until the pressure-volume relationship became non-linear (i.e., small increments of volume causing a large increase in pressure). Starting from this point, defined as the maximal inflation point, volume was withdrawn from the lungs in small steps until the minimal point (resting volume) was reached. Thirty seconds were allowed for equilibration during each step before tracheal pressure was recorded. This procedure has been employed in the literature to obtain a pulmonary volume (PV) curve (4-6). For experiments with fluid-filled lungs, saline was injected through the cannula and the same procedure was repeated.


Figure 1 - Schematic representation of the system used to construct the PV curve for the excised rat lungs.


Respiratory work estimation

The effects of paraquat were computed by integrating the PV curve area at inflation and deflation to obtain the inspiratory and expiratory work, respectively. An estimator of tissue work corresponds to the integration of the PV curve obtained with saline. Results are reported as work/ml of volume displacement, i.e, by dividing the areas of the PV curve by the corresponding overall variation of volume.

Statistical analysis

Values are reported as means ± SEM. The statistical significance of tissue and tension works/ml was determined by ANOVA with a P value <0.05 accepted as significant, with post hoc assessment of differences by means of the Student-Newman-Keuls test. Logarithmic transformation of the measured variables was employed in order to stabilize variance.


Results

Respiratory work

Figure 2 shows representative PV curves obtained in air-filled lungs of a control rat (number 4) and in a 25-mg/kg weight paraquat-intoxicated (number 1) rat. There was a shift to the right of the inspiratory limb as well as an increase in the area of hysteresis in the paraquat-intoxicated animal. The differences in hysteresis between control and paraquat-intoxicated animals virtually disappeared in the saline-filled lungs (Figure 3). Interestingly enough, the animal treated with paraquat was able to receive a larger amount of volume in comparison to the control rat. Although this behavior was not observed for all paraquat-treated animals, this finding may suggest that tissue viscoelastic properties might be somewhat affected in some animals by the shear stress caused by previous air breathing in a context of mechanical instability. Nonsignificant changes of tissue elasticity were observed for all doses of paraquat employed, whereas inspiratory work due to surface properties exhibited a dose-dependent increase (Table 1 and Figure 4). Expiratory work was also significantly elevated in the 50-mg/kg body weight paraquat-intoxicated group (Table 2 and Figure 5).


Figure 2 - Static pressure-volume curves obtained in air-filled lungs from a control rat and a paraquat (25 mg/kg body weight)-intoxicated rat. The inspiratory limb was shifted to the right in the paraquat-treated animal. In addition, hysteresis was markedly increased after paraquat treatment.

[View larger version of this image (10 K GIF file)]


Figure 3 - Static pressure-volume curves obtained for saline-filled lungs of a control rat and a paraquat (25 mg/kg body weight)-intoxicated rat. Hysteresis was similar in both animals. Interestingly enough, the paraquat-treated animal was able to receive a larger amount of volume in comparison to the control rat.

[View larger version of this image (10 K GIF file)]


Figure 4 - Mean values (circles) and corresponding standard errors (lines) of the 95% confidence interval (CI) of inspiratory work attributable to surface tension and tissue forces in control animals and in animals submitted to different doses of paraquat (Pq) intoxication.

[View larger version of this image (10 K GIF file)]


Figure 5 - Mean values (circles) and corresponding standard errors (lines) of the 95% confidence interval (CI) of expiratory work attributable to surface tension and tissue forces in control animals and in animals submitted to different doses of paraquat (Pq) intoxication.

[View larger version of this image (9 K GIF file)]


Discussion

The degree of paraquat poisoning depends on the amount used; however, the most characteristic feature is lung damage, which is usually the cause of death. Paraquat produces oxygen-derived free radicals and severely injures the lungs by accumulating in type II pneumocytes. This lesion suggests that paraquat may decrease surfactant production besides increasing microvascular permeability that leads to acute protein-rich edema formation. Individuals surviving this acute phase usually show a period of improvement, which is the prelude to irreversible lung damage. Smith et al. (7) have described the pathogenesis and structure of paraquat-induced fibrosis in rats following acute and chronic administration, using doses from 20 to 100 mg/kg body weight. They demonstrated that in the development of the irreversible lesion there is an early stage of edema and disintegration of pulmonary epithelium, followed by an infiltration of profibroblasts resulting in intra-alveolar fibrosis. In the first phase, there is also a destructive effect on type I and type II pneumocytes with formation of edema and infiltration of inflammatory cells, characterizing the presence of alveolitis. The second phase, if death did not occur in the acute state, is a reparative lesion with extensive fibrosis of the alveolar tissue, that may also lead to death from hypoxia.

Many theories have been proposed to describe the effect of interface tensions on the alveolar surface and the ability of the alveoli to coexist in a stable configuration. The surface tension due to elastic fibers and to the air-liquid interface forces the lung to collapse and a surfactant antagonizes this recoil pressure. It is well established that a high surface tension within air spaces tends to make them collapse, and that a low surface tension conferred by a surfactant is necessary if alveoli are to remain expanded at low lung volumes (8).

Hysteresis is the property whereby the pressures exerted by elastic recoil of the respiratory system are greater on inflation (inspiration) than on deflation (expiration) at the same volumes (9). A given volume must be shared by a smaller number of alveoli (or alveoli of smaller size) during inflation than during deflation, and therefore pressures during the inspiratory phase are higher than at expiration, completing a volume-pressure hysteresis loop. The area inside the static PV loop is indicative of the energy dissipated within the pulmonary parenchyma (10). This area has the dimension of work and is properly regarded as a component of the elastic work required to inflate the respiratory system. Since the critical opening pressure is inversely proportional to alveolar unit size, it follows that progressive recruitment of air spaces requires a continuously increasing pressure during inflation, which leads to high peak inspiratory pressures. Unpleating of alveolar walls and distention of septa also contribute to increments in inspiratory pressure (11). The inflation curve of the excised lung exhibits a "knee" on the inflation limb, meaning that rapid and nearly complete recruitment of lung units occurs at the "inflection point" of the curve. The PV curve allows analysis of the pulmonary surface forces since the difference between air-filled and saline-filled lungs is considered to be a result of surface tension. The tissue component of recoil pressure in the air-filled lung (deflation path) is similar to that of the saline-filled lung at the same volume (12). There is currently no standardized procedure for the construction of lung PV curves, and their shape may vary among different species (6).

The results of the present study indicate that acute paraquat intoxication in rats causes pulmonary lesions mainly due to surfactant dysfunction, sparing lung tissue, as shown in the PV curves obtained for air- and saline-filled lungs (Figures 2 and 3). Other models of acute lung injury have been described and have confirmed the effectiveness of the PV curve to study pulmonary mechanics (13,14). Both tension work and hysteresis loop were greater in the paraquat group, and the extent of alteration increased as larger doses were administered (Figure 4). In the inspiratory limb, pressures were much higher in the paraquat lung since the degree of collapse due to surfactant dysfunction was intense. Hysteresis was almost eliminated in the saline-filled lung in both groups, since it was mainly due to an alveolar surface film. Alterations of work due to surface active properties were observed both during inspiration and expiration. However, inspiratory work due to tension was different from control starting at the lowest dose of paraquat. Expiratory work due to tension changed significantly only at the highest dose of paraquat (Figure 5). These results suggest that inspiratory tension work is a more sensitive estimator of alveolar instability in paraquat poisoning.

Therefore, paraquat poisoning, as demonstrated here, presents a useful model of respiratory insufficiency similar to acute lung injury. In addition, the degree of pulmonary dysfunction was shown to be dependent on drug dose. This finding indicates that paraquat intoxication represents a suitable model to induce alveolar instability of different magnitudes to be used in further studies of mechanical ventilation.


References

1. Lewis C & Nemery B (1995). Pathophysiology and biochemical mechanisms of the pulmonary toxicity of paraquat. In: Bismuth C & Hall AH (Editors), Drug and Chemical Toxicology. Paraquat Poisoning. Marcel Dekker, New York.         [ Links ]

2. Delaval PM & Gillespie DJ (1985). Pulmonary dysfunction during paraquat-induced lung injury: A model of acute alveolar injury. Critical Care Medicine, 13: 1056-1060.         [ Links ]

3. Manieri R, Bronzi R, Grilli A, Loffredo B, Data PG, Napolitano L & Felaco M (1990). Effect protecteur de l'hypoxygénation hyperbarique au cours de l'intoxication par le paraquat, chez le rat. Journal du Toxicologie Clinique et Experimentale, 10: 297-305.         [ Links ]

4. Bachofen H, Schürch S, Urbinelli M & Weibel ER (1987). Relations among alveolar surface tension, surface area, volume, and recoil pressure. Journal of Applied Physiology, 62: 1878-1887.         [ Links ]

5. Sharp JT, Johnson FN, Goldberg NB & Lith PV (1967). Hysteresis and stress adaptation in the human respiratory system. Journal of Applied Physiology, 23: 487-497.         [ Links ]

6. Lum H & Mitzner W (1987). A species comparison of alveolar size and surface forces. Journal of Applied Physiology, 62: 1865-1871.         [ Links ]

7. Smith P, Health D & Kay JM (1974). The pathogenesis and structure of paraquat-induced pulmonary fibrosis in rats. Journal of Pathology, 114: 57-67.         [ Links ]

8. Mead J, Takashima T & Leith D (1970). Stress distribution in lungs: a model of pulmonary elasticity. Journal of Applied Physiology, 28: 596-608.         [ Links ]

9. Mead J, Whittenberger JL & Radford Jr EP (1957). Surface tension as a factor in pulmonary volume-pressure hysteresis. Journal of Applied Physiology, 10: 191-196.         [ Links ]

10. Robatto FM, Romero PV, Fredberg JJ & Ludwig MS (1991). Contribution of quasi-static tissue hysteresis to the dynamic alveolar pressure-volume loop. Journal of Applied Physiology, 70: 708-714.         [ Links ]

11. Mercer RR, Laco JM & Crapo JD (1987). Three-dimensional reconstruction of alveoli in the rat lung for pressure-volume relationships. Journal of Applied Physiology, 62: 1480-1487.         [ Links ]

12. Wilson TA (1982). Surface tension-surface area curves calculated from pressure-volume loops. Journal of Applied Physiology, 53: 1512-1520.         [ Links ]

13. Coker PJ, Hernandez LA, Peevy KJ, Adkins K & Parker JC (1992). Increased sensitivity to mechanical ventilation after surfactant inactivation in young rabbit lungs. Critical Care Medicine, 20: 635-640.         [ Links ]

14. Jackson JC, Standaert TA, Truog WE, Murphy JH, Palmer S, Chi EY, Woodrum DE, Watchko JF & Hodson WA (1985). Changes in lung volume and deflation stability in hyaline membrane disease. Journal of Applied Physiology, 59: 1783-1789.         [ Links ]


Correspondence and Footnotes

Address for correspondence: Correspondence

P.H.N. Saldiva, Departamento de Patologia, Faculdade de Medicina, USP, Av. Dr. Arnaldo, 455, 01246-903 São Paulo, SP, Brasil. Fax: 55 (011) 3064-2744. E-mail: pepino@usp.br

Research supported by CAPES. Publication supported by FAPESP. Received July 22, 1997. Accepted January 12, 1998.

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