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<br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br /> <br />Impacts of Electrofishing on Fish <br /> <br />electrofishing operation (like people working on a <br />metal boat used as the cathode). The level of <br />ambient potential relative to the electrodes depends <br />on the power output, total resistance (sum of anodic <br />and cathodic resistances), and the ratio of anodic to <br />cathodic resistance. When cathodes are much larger <br />than anodes, most of the total potential between <br />electrodes is associated with the anode, the voltage <br />differential between ambient potential and the <br />cathode is relatively small, and voltage gradients near <br />the cathode are much lower than near the anode. <br />The size, shape, configuration (e.g., single or <br />multiple electrode arrays) and relative position of the <br />electrodes should be selected according to the <br />available power output, water conductivity, and <br />desired distribution of current in the water. Novotny <br />(1990) emphasized that "The most common electrode <br />problem is that the electrodes are simply too small . <br />. . ." At the same voltage output, the larger the <br />electrode, the less its electrical resistance in water, <br />the lower the maximum field intensity immediately <br />around it, the smaller the zone of tetany , and the <br />larger the effective field (greater the range). <br />Sometimes the zone of tetany can even be <br />eliminated. Increasing the number of anodes or <br />cathodes in a system has a cumulative effect similar <br />to increasing the size of an individual electrode (the <br />effect is maximized when multiple electrodes are <br />well separated). Maximum size or number of anodes <br />or cathodes is dictated largely by practical <br />considerations (e.g., maneuverability, transportability, <br />interference with netting). It can also be limited by <br />the maximum power output of the generator, <br />especially in highly conductive waters. Electrode <br />resistance varies inversely with either electrode size <br />(available surface area) or water conductivity. At <br />constant applied voltage, reductions in total electrical <br />resistance result in increased current, sometimes <br />enough to overload the generator. When water <br />conductivity is high, the size of the electrodes must <br />sometimes be reduced to prevent such an overload. <br />Spherical electrodes are generally considered <br />superior to other shapes (e.g., cables or narrow <br />cylinders). Electric fields generated immediately <br />around spheres are uniform and without the hot spots <br />(localized regions of higher intensity) produced near <br />the corners and edges of many other electrode <br />shapes. Novotny and Priegel (1974) and Novotny <br />(1990) noted that except near their surfaces, circular <br /> <br />Review I Electric Fields in Water 17 <br /> <br />and ring-like electrodes, including dropper arrays, <br />produce fields similar to those produced by spheres. <br />In DC and PDC systems, the desired <br />electrofishing responses are generally produced only <br />in anodic fields, whereas fish tend to be repulsed by <br />cathodic fields. However, some adverse effects may <br />be as great or greater in cathodic fields. Jesien and <br />Hocutt (1990) found that channel catfish in <br />homogeneous fields are more sensitive to tetany <br />when facing the cathode than when facing the anode. <br />To minimize cathodic effects on fish, cathodes <br />should be as large as practical. As noted above, this <br />will also maximize potential in the anodic field and <br />reduce the overall electrical resistance of the system. <br />In systems with cathodes much larger than anodes, <br />the very low voltage differential between the cathode <br />and soil and water in vicinity reduces the risk of <br />severe shock or electrocution to people or animals <br />that inadvertently approach or touch the cathode <br />(Smith 1989). Because cathodic resistance for well <br />separated electrodes is halved each time the surface <br />area of the cathode is doubled, Smith (1989) <br />suggested that 10 m2 is a practical limit to the size of <br />the cathode. <br /> <br />Electrofishing Currents and Waveforms <br /> <br />Electrical currents are of two principal types: <br />bipolar or alternating currents characterized by <br />continually reversing polarity and movement of <br />electrons (AC; Figure 9A) and unipolar or direct <br />currents characterized by movement of electrons in <br />one direction. More specifically, the term DC refers <br />to unipolar currents that are continuous and relatively <br />constant in voltage (Figures 9B, 9C). Both AC and <br />DC can be periodically interrupted or pulsed. <br />Although pulsed AC (e.g., Jesien and Hocutt 1990) <br />is seldom used for electrofishing, several variations <br />of pulsed DC (PDCs) are very popular and typically <br />used with boat systems. PDCs are characterized by <br />frequency (Hz-Hertz, cycles or pulses per second), <br />pulse width (time power is applied during each pulse <br />cycle, usually expressed in ms, milliseconds) or duty <br />cycle (time power is applied per cycle, expressed as <br />a percent of cycle time), shape or waveform (e.g., <br />rectangular, exponential, half sine, and quarter sine), <br />and pattern (either a uniform frequency or <br />secondarily interrupted at much slower frequencies to <br />produce bursts, packets, or trains of pulses). The <br />