scholarly journals The Electric Sense of Sharks and Rays

1971 ◽  
Vol 55 (2) ◽  
pp. 371-383 ◽  
Author(s):  
A. J. KALMIJN

1. Previous experiments have demonstrated that (a) the shark Scyliorhinus canicula and the ray Raja clavata are extremely sensitive to weak electric fields; (b) their electrical sensitivity is due to the ampullae of Lorenzini; (c) the sharks and rays can be stimulated by the bioelectric fields emanating from the flatfish Pleuronectes platessa. 2. When hungry, Scyliorhinus and Raja perform well-aimed feeding responses to flatfish, even if the prey have covered themselves with sand. The object of the present study was to determine whether the sharks and rays use the bioelectric fields of the flatfish to detect the position of their prey. 3. To analyse the feeding responses of the sharks and rays, a flatfish was put into an agar chamber. The predators responded to the so screened prey from the same distance, and tried to feed on it in the same way as if there were no agar at all. As the flatfish in the agar chamber was completely hidden from view, the sharks and rays were thus shown not to need visual contact to locate the prey. 4. If the agar chamber was filled with cut-up pieces of whiting, the sharks and rays did not respond to the food, although the odour of whiting juice normally attracts them strongly. Therefore, the sharks and rays did not detect the position of the agarscreened flatfish by smell. 5. The feeding responses to the flatfish could be entirely abolished by covering the agar chamber with a very thin sheet of plastic. The mechanical attenuation offered by the plastic film was too weak to explain its dramatic inhibitory effect, and, thus, a purely mechanical detection of the agar-screened flatfish without plastic film was also ruled out. 6. As the responses to the agar-screened flatfish were not merely due to visual, chemical, or mechanical stimuli, it was tentatively concluded that the sharks and rays perceived the prey electrically. This conclusion was fully in agreement with the results of the experiments, for the agar chamber did not appreciably distort the bioelectric fields of the flatfish, and the electrical impedance of the plastic film was extremely high. 7. Further, the bioelectric field of a flatfish was simulated with a pair of electrodes, buried in the sand. Now, the sharks and rays displayed exactly the same feeding responses to the electrodes as they did previously to the real prey. This crucial experiment confirmed the electrical hypothesis in a very direct way. 8. The experiments described demonstrate clearly that the shark Scyliorhinus canicula and the ray Raja clavata make a biologically significant use of their electrical sensitivity. Therefore, we now are justified in accrediting the animals with an electric sense and in designating the ampullae of Lorenzini as electroreceptors. 9. When the sharks and rays were offered a piece of whiting in the vicinity of two electrodes simulating a flatfish, they were attracted by the odour of the food but usually performed their well-aimed responses to the electrodes. Thus, at short range, the electric fields act as a much stronger directive force than do the visual and chemical stimuli. Only direct mechanical contact dominates over the electrical stimuli. 10. Theoretically, the sharks and rays can detect the electric fields resulting from ceanic and tidal currents. Whether they make use of the available information for orientation in the open sea is not yet known. Furthermore, the observations and measurements described indicate that, in studying shark attacks, the electric fields of the prey and the electric sense of the predators should be taken into account.

2013 ◽  
Vol 2 (2) ◽  
Author(s):  
Fauzi Akbar ◽  
Zulisma Anita ◽  
Hamidah Harahap

Biodegradable plastics are plastics that will decompose in nature with the help of microorganisms. The use of starch as the main material of plastic manufacturing has great potential because in Indonesia there are different starch crops. To obtain bioplastics, starch is added to the plasticizer glycerol, in order to obtain a more flexible plastic and elastic. This study reviews the use of cassava starch and glycerol skin as a base for the manufacture of biodegradable plastics. The purpose of this research is to know the effect of storage time on the mechanical properties of plastic film biodegradation of starch cassava peel. The results obtained in the form of a thin sheet plastic film that have been tested mechanical properties such as tensile strength, elongation at break, and elasticity. Mechanical properties of plastic films will decrease every week due to the absorption of moisture and plasticizer migration occurs in a matrix of plastic films for storage.


2016 ◽  
Vol 2 (5) ◽  
pp. e1600112 ◽  
Author(s):  
Erik E. Josberger ◽  
Pegah Hassanzadeh ◽  
Yingxin Deng ◽  
Joel Sohn ◽  
Michael J. Rego ◽  
...  

In 1678, Stefano Lorenzini first described a network of organs of unknown function in the torpedo ray—the ampullae of Lorenzini (AoL). An individual ampulla consists of a pore on the skin that is open to the environment, a canal containing a jelly and leading to an alveolus with a series of electrosensing cells. The role of the AoL remained a mystery for almost 300 years until research demonstrated that skates, sharks, and rays detect very weak electric fields produced by a potential prey. The AoL jelly likely contributes to this electrosensing function, yet the exact details of this contribution remain unclear. We measure the proton conductivity of the AoL jelly extracted from skates and sharks. The room-temperature proton conductivity of the AoL jelly is very high at 2 ± 1 mS/cm. This conductivity is only 40-fold lower than the current state-of-the-art proton-conducting polymer Nafion, and it is the highest reported for a biological material so far. We suggest that keratan sulfate, identified previously in the AoL jelly and confirmed here, may contribute to the high proton conductivity of the AoL jelly with its sulfate groups—acid groups and proton donors. We hope that the observed high proton conductivity of the AoL jelly may contribute to future studies of the AoL function.


If a parallel pencil of homogeneous β -rays is made to fall on a thin sheet of any material the individual β -particles are deflected from their original path and the beam becomes scattered or diffuse. The deflections may be very considerable, even when the thickness of the material is far too small to produce any appreciable absorption either in the number or the energy of the particles in the beam. These deflections are generally ascribed to the action of the strong electric fields within the atoms of the scattering material, and measurements on the scattering of the rays afford a useful means of investi­gating the nature and magnitude of these atomic fields. Experiments on the scattering of a beam of homogeneous β -rays were made some years ago by one of the writers with the object of obtaining an estimate of the number of electrons in the atoms of different elements. A theory of the phenomenon had been previously put forward by Sir J. J. Thomson on the assumption, which was then generally accepted, that the atom consisted of a number, N, of negative electrons embedded in a sphere of positive electri­fication of atomic radius. On this view the deflection of a β -particle may be due either to the repulsion of the negative electrons in the atom, or to the attraction of the positive sphere. The probability of a particle suffering a large deflection from either of these causes could be shown to be negligibly small, and the actual observed deflections to be due to the cumulative effects of a large number of small deflections. Applying a theorem due to Lord Rayleigh it was shown that the probability that the deflection of the particle should be less than a given angle Ф was equal to where is the 1 - ϵ - Ф 2 / kt thickness of the scattering material, and k a constant which depends on the nature of the substance and the energy of the rays. Thus, if the rays after passing through the scattering substance were limited by a circular stop, whose radius subtended an angle Ф at the substance, the intensity of the radiation passing through the stop should be given by I/I 0 = 1 - ϵ - Ф 2 / kt , where I 0 is the initial intensity of the beam.


2017 ◽  
Vol 157 ◽  
pp. 31-37 ◽  
Author(s):  
Ramon Novoa-Carballal ◽  
Ricardo Pérez-Martín ◽  
María Blanco ◽  
Carmen G. Sotelo ◽  
Dario Fassini ◽  
...  

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