Experimental models of brain injury

General categories of experimental brain injury models are reviewed regarding their clinical significance, and two new models are presented that use different methodology to produce injury. This report describes and characterizes the pathophysiologic changes produced by a novel fluid percussion (FP) method and a controlled cortical impact (CI) technique, both developed at the General Motors Research Laboratories (GMRL). The new models are compared to prior experimental brain injury techniques in relation to ongoing physical and analytical modeling used in automotive safety research by GMRL. Experimental results from our laboratory indicate that although the FP technique, currently the most widely used method for producing brain injury, is useful for producing graded injury responses systemically and centrally, it is not well-suited for detailed biomechanical analyses. This conclusion is based on high-speed cineradiographic studies where the physiologic saline in the FP cannula was substituted with a radiopaque contrast medium (Conray 1:1 dilution/saline). High speed x-ray movies (1000 fps) were taken of the fluid percussion pulse (1.5-3.4 atm/20 msec) in sagittal, dorsal, and frontal planes of orientation. When viewed together, the cineradiography revealed a complex, dynamic interaction between the injected fluid and the skull/cranial contents. Rapid lateral and anterior/posterior epidural fluid flow suggest that the pathology and dysfunction following FP brain injury reflects diffuse mechanical loading of the brain. Because fluid is used to transfer mechanical energy to brain tissue, and because fluid flow characteristics (i.e., direction, velocity, and displacement) are dependent on the brain geometry and species used, accurate analytical and biomechanical analyses of the resultant injury would be difficult at best. In contrast, the cortical impact model of experimental brain injury uses a known impact interface and a measurable, controllable impact velocity and cortical compression. These controlled variables enable the amount of deformation and the change in deformation over time to be accurately determined. In addition, the CI model produces graded, reproducible cortical contusion, prolonged functional coma, and extensive axonal injury, unlike the FP technique. The quantifiable nature of the single mechanical input used to produce the injury allows correlations to be made between the amount of deformation and the resultant pathology and functional changes.(ABSTRACT TRUNCATED AT 400 WORDS)     

A study of galactose intolerance in human and rat liver in vivo by 31P magnetic resonance spectroscopy.

An oral load of 20 mg/kg galactose produces significant changes in the 31P magnetic resonance spectrum of the liver of a galactosemic patient. The peak at 5.2 ppm (which includes inorganic phosphate and galactose-1-phosphate) increased on two occasions to about twice its original size 60 min after galactose administration. An oral load of 10 mg/kg galactose given to a second patient produced no discernible changes at 30 min. We have also used an animal model of galactose intolerance, in which galactose metabolism in rats was blocked by the acute administration of ethanol. Studies in vivo and in vitro showed that the increase in the peak at 5.2 ppm was largely due to galactose-1-phosphate. We have shown in this preliminary study that small amounts of galactose can produce significant elevation of hepatic galactose-1-phosphate, which can be detected by 31P magnetic resonance spectroscopy.     

Physiologic, histopathologic, and cineradiographic characterization of a new fluid-percussion model of experimental brain injury in the rat

The fluid-percussion technique produces experimental brain injury by rapid injection of a fluid volume into the closed cranial cavity. The experiments reported here characterize a new, more controlled technique for fluid-percussion brain injury in the rat and systematically examine systemic physiologic, histopathologic, and electroencephalographic responses in the rat at two levels of injury severity. The new technique was developed to permit independent variation of the fluid pressure pulse parameters and, thus, more accurately define the brain loading conditions associated with fluid-percussion injury. The new technique produced changes in mean arterial blood pressure similar to previous techniques; however, bradycardia was not observed. Significant increases in heart rate were produced by both injury levels and were more prolonged at the high level of injury severity. Both magnitudes of injury produced significant decreases in EEG amplitude immediately postinjury, but high severity injury produced a greater decrease in delta frequency band (1-4 Hz) activity than did low severity injury. Both levels produced hemorrhage at the site of injury, thalamus, corpus callosum, hippocampus, and fimbria hippocampus similar to previous techniques. Higher levels of injury produced more extensive cerebral hemorrhage and greater spinal involvement. In a separate group of animals, cineradiographic images were made at coronal, sagittal, and dorsal orientations during the fluid pressure pulse. Intracranial fluid movement was characterized by rapid radial movement within the epidural space. The data suggest that the distributed nature of fluid-percussion induces pathology, and dysfunction may reflect a diffuse mechanical loading of the brain surface. The model appears to give repeatable effects useful in the study of closed head injury.     

Copper vapor laser fragmentation of gallstones: in vitro measurements of wall heat transmission

Laser fragmentation is a promising new modality in management of retained CBD stones. Recent reports demonstrate the feasibility of lasers for this, but few studies have evaluated their safety (e.g., thermal injury may occur at greater than 43 degrees C). This study was conducted to measure heat transmission from lased bilirubinate and mixed stones to a simulated CBD wall. Four welded thermocouples were passed to the inside wall of 6-mm polyvinyl tubing 90 degrees apart to surround the lumen stone. The thermocouples were interfaced to a computer and temperatures were recorded every 270 msec. The tubing was submerged in a 37 degrees C water bath for all lasing work. A copper vapor laser (wavelength, 510 nm; 5.6 W; 5 kHz; pulse length, 30 ns) was attached to a 650-micron quartz fiber. A stone was "impacted" in the tubing and the laser fiber was pushed against the stone while making multiple passes to fragment it. Thirty mixed gallstones (mean size, 6.9 X 5.1 mm) and 20 bilirubinate gallstones (mean size, 7.1 X 5.2 mm) were fragmented during the study. Maximum temperature (Tmax), duration of Tmax (TmaxD), interval to stone piercing (TiP), and interval to fragmentation (TiF) were measured and comparisons were carried out with the SPSS statistical package using the t test procedure. The Tmax generated during fragmentation of bilirubinate stones (43.4 +/- 1.7 degrees C) was significantly less (P less than 0.002) than the Tmax for mixed stones (54.0 +/- 2.7 degrees C) but both Tmax values represented potentially injurious temperature levels.(ABSTRACT TRUNCATED AT 250 WORDS)