Intensity fluctuation spectroscopy was used to detect particle motion within the pericardial organ of the crab Carcinus while it was perfused with media with increased potassium concentrations. Replacement of some or all of the sodium ions of the normal medium with potassium ions caused a graded increase in motion. Evidence is presented which indicates that this effect is not a consequence of membrane depolarization or calcium ion influx, but is due to the flux of potassium chloride and water into the cytoplasm of the cells. The observation of Shaw and Newby has been confirmed and extended by Piddington and Sattelle (5). They found, however, that omission of calcium ions from the medium had no effect on the potassium response (6). Despite this, they nevertheless attributed the scattering change to calcium entry.We have investigated this phenomenon to determine whether it has any relevance to the mechanism of neurotransmitter release. The pericardial organ of the crab Carcinus was used. This is a specialized neurosecretory structure, the cortex of which is packed tightly with neurosecretory endings containing a variety of granules and vesicles (7). It usually has a bluish color when viewed under a dissecting lamp, probably due to light scattering by the granular inclusions of the nerve endings (8).
METHODSSpecimens of Carcinus were obtained from the Marine Biological Laboratory at Woods Hole and kept in a tank of artificial sea water at about 15'C. The pericardial organ was dissected from an animal in artificial sea water and transferred to a microscope slide to which it was fastened with Vaseline. The microscope slide formed the bottom of a perfusion chamber which could be covered and sealed with a cover slip. This chamber was then mounted on the stage of a specially modified Zeiss WL microscope (Fig. 1).This microscope permits observation of preparations with the incandescent illuminator of the microscope as well as with laser light. The beam of a 4-mW He/Ne laser (Coherent Radiation model 80) passes through a lens and is reflected from a half-silvered mirror and focused onto the back focal plane of the microscope condenser (numerical aperture = 1.4). The beam then passes through the preparation at an angle determined by the lateral displacement of the beam off the optical axis of the microscope (9). This angle can be adjusted between 0°and almost 90°by means of the micrometer drive on the lens-mirror assembly.An iris diaphragm in the image plane of the microscope can limit the field to an area 27 gam in diameter (using a 40X objective). This diaphragm and the image of the preparation can be observed through an ocular or, by removing a mirror from the system, the light scattered from the preparation can be passed through a pair of lenses that bring the back focal plane of the microscope objective (40X, numerical aperture = 0.65) to focus on an aperture in front of the cathode of a photomultiplier tube. The position of this aperture in the back focal plane determines the angle at which light is collected...