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c ( r / a ) } = a 2 π J 1 ( 2 π a p ) π a p ,   (3) Where &Jai_unknown_entity_euclidsymbol_F072; is a radial coordinate in the plane of the observation and J 1. is the first order Bessel function of the first kind. The amplitude distribution in the

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power and D s ( τ ) is the geometric function given by the relation 27 in which L 0 is the modified Bessel function and l , k are the dimension of the resistive pattern. To record the potential difference variations, which normally are

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