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Last modified
7/14/2009 5:01:44 PM
Creation date
5/22/2009 12:26:56 PM
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Template:
UCREFRP
UCREFRP Catalog Number
7116
Author
Baxter, G. and J. Simon
Title
Editor
USFW Year
Series
USFW - Doc Type
1970
Copyright Material
YES
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<br /> .... <br />. ..... 0 <br /> 0 ..... 0 <br /> '... <br /> 0 -... <br /> 0 0 -- <br /> . --- --- <br />0.1 . <br /> . <br /> ~.. . <br /> . . <br /> . <br /> . <br /> . . <br /> . . <br /> ." ..~ <br /> . . <br /> . . . <br /> . <br />0.0 <br />0 10 20 30 40cm <br /> LENGTH <br /> <br />I' <br />j <br /> <br />V/cm <br /> <br />3.0 <br /> <br />>- <br />I- 1.0 <br />Ci.i <br />Z <br />w <br />o <br />w <br />z <br />:J <br />I- <br />Z <br />W <br />0: <br />0: <br />::> <br />() <br /> <br /> <br />o <br /> <br />13 <br /> <br />o <br /> <br />DIRECT CURRENT = - - - - - <br />ALTERNATE CURRENT - - <br /> <br />. <br /> <br />o <br /> <br /> <br />Fig. 4, Current line density needed for attraction of different fish species with direct and alternating current (data from Steroio <br />el al., 1972). <br /> <br />attracting the fish. By choosing the proper output <br />effect, the zone of attraction can therefore be <br />larger with constant than with pulsed direct <br />current. The total fishing zone (including the <br />immobilization zone) is, however, always larger <br />with pulsed direct current. The former case might <br />under certain circumstances be advantageous. <br />The physiological effect of pulsed direct current <br />is. positively correlated with both frequency <br />(Sternin et al., 1972; Hickley, 1985) and pulse <br />length and is related to the duty cycle (fre- <br />quency x pulse length) according to a power <br />function (Fig. 5). With a duty cycle exceeding 0.2 <br />(1.0 = constant current) the effect of pulsed cur- <br />rent surpasses that of constant current. The field <br />strength needed for immobilisation is asymptoti- <br />cally reaching a minimum value at higher fre- <br />quences (for roach 0.2 vfcm at frequencies> 50 <br />Hz; Hickley, 1985). <br /> <br />When increasing the pulse length the attraction <br />radius of the anode will asymptotically reach a <br />value, which is dependent upon frequency, fish <br />size and water conductivity. This value varies <br />between 0.1 and 5 mS (Vibert, 1967; Sternin <br />et aI., 1972). As, however, the effect needed in- <br />creases linearly with the pulse length, an optimum <br />pulse length (considering fishing efficiency and <br />energy consumption) of 0.5-1.0 mS (10-40 Hz) <br />is achieved. <br />The effect of varying the shape of the pulse is <br />largely unknown. Vibert (1967) states, that con- <br />denser pulses (having a fast voltage increase and <br />a slow decrease, cf. Fig. 2f) produce the largest <br />effects. Sterninet al. (1972), however, were unable <br />, <br />to find any empirical evidence for this statement. <br />The size and the material of the electrodes <br />determine the current line density and the strength <br />and corrosion resistance of the electrodes. <br />
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