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<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
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