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North American Journal of Fisheries Management 8:516-518, 1988 <br /> <br />f <br />r. ; <br />0 <br />2i <br />Y: <br />;i <br />S <br />COMMENTS <br />Electrofishing Injury to Large Rainbow Trout <br />Sharber and Carothers (1988) recently evalu- <br />ated the effect of three wave forms of pulsed DC <br />on spinal injury to large (300-560 mm, total length) <br />rainbow trout Oncorhynchus mykiss (formerly <br />Sabno gairdneri) captured by electrofishing in the <br />Colorado River. They reported an overall injury <br />incidence of 50% and a significantly higher inci- <br />dence in fish stunned with a quarter-sine wave <br />(67%) than in those captured with either expo- <br />nential or square waves (44% each). Although <br />Sharber and Carothers focused their study on the <br />comparison of the three wave forms, they recog- <br />nized a more important conclusion from their re- <br />sults: large rainbow trout are very susceptible to <br />injury induced by any form of pulsed electroshock. <br />Indeed, Hauck (1949) reported that 26% of 503 <br />large rainbow trout (he gave no size range for his <br />sample, but mentioned weights of 0.7-2.3 kg) died <br />within 2-5 d after they were exposed to AC; the <br />incidence of injuries was not stated but probably <br />was much higher. Other studies of electroshock <br />injury to rainbow trout, cited by Sharber and Car- <br />others, showed lower injury incidence; however, <br />these studies were conducted on smaller fish or in <br />less-conductive water, which could account for the <br />lower incidence. <br />Although Sharber and Carothers appropriately <br />cautioned biologists about electroshocking large <br />rainbow trout, they offered no explanation for the <br />alarming incidence of injury or recommendations <br />for addressing the problem. We believe an expla- <br />nation and appropriate countermeasures exist, and <br />herewith offer them for consideration. <br />Given the electrodes (two spheres, 30 cm in di- <br />ameter), peak voltage (260 V), and water conduc- <br />tivity (about 700,uS/cm) described by Sharber and <br />Carothers, one can calculate the intensity of the <br />electrical field. Because the water conductivity of <br />700,uS/cm is specific to 25°C (N. Sharber, personal <br />communication), it must be recalculated to 10°C, <br />the water temperature at capture, by assuming a <br />2% conductivity change for every 1°C between 10 <br />and 25°C: 700/1.0211- 10 = 520 AS/cm. If one uses <br />the equation given by Novotny and Priegel (1974), <br />the resistance (R) of one electrode is R =1(y)/Ka' <br />= 0.159/30(0.00052) = 10.2Q; fly) is a dimension <br />constant for spheres, Kis the sphere diameter (cm), <br />0) 1 t,3 <br />ti is 10-6v, and a is the water conductivity in µS/ <br />cm. There are two identical electrodes in series, <br />so their combined resistance is the sum of their <br />individual resistances or 20.452. By Ohm's Law, <br />therefore, the current at peak voltage is I = volt- <br />age/resistance = 260/20.4 = 12.7 A. <br />Next, one calculates voltage gradient at the elec- <br />trode surface (Novotny and Priegel 1974) as <br />E = 11[4av'r2] <br />= 12.7/[(4rr)0.00052(15)2] <br />= 8.6 V/cm; <br />r is the radius (cm) of the electrode. If 8.6 V/cm <br />occurs at 0 cm from the electrode surface (i.e., <br />when r = 15 cm), E at 10, 50, and 100 cm (r = <br />25, 65, and 115 cm, respectively) is 3.1, 0.5, and <br />0.15 V/cm. Thus, E is highest at the electrode <br />surface and decreases nonlinearly with distance to <br />one-tenth of maximum within 0.5 in of the elec- <br />trode. Our estimate of voltage gradient may be <br />low because the electrodes are used in shallow water <br />where the boundary layers (water surface and sub- <br />strate) tend to intensify the electrical field. <br />We believe that the critical parameter for de- <br />scribing electrofishing effectiveness is power den- <br />sity (Kolz and Reynolds, unpublished data). Power <br />density at any point in an electrofishing field can <br />be calculated by the equation µW/cm' = QE'-. Thus, <br />at the surface of the Sharber-Carothers electrode, <br />power density was 38,459 µW/cm3, and was 4,997, <br />130, and 12 µW/cm' at 10, 50, and 100 cm from <br />the electrode. For reference, the minimum (thresh- <br />old) power density required to narcotize, without <br />injury, goldfish Carassius auratus under controlled <br />conditions was 100-180 µW/cros, depending on <br />whether DC, pulsed DC, or AC was used (Kolz <br />and Reynolds, unpublished data). <br />More relevant to the issue at hand are the results <br />of recent studies by the Alaska Department of Fish <br />and Game (ADFG), which corroborated the find- <br />ings of Sharber and Carothers (D. McBride, ADFG, <br />personal communication). Among electroshocked <br />rainbow trout (N = 22; fork length, >400 mm) <br />from the Kenai River (a = 50 µS/cm at 7°C), the <br />incidence of spinal injury was 50%. 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