For the short dipole with length l such that l

For the short dipole with length l such that l

For the short dipole with length l such that l < ?,=”” instead=”” of=”” treating=”” the=”” current=”” i=”” (z)=”” as=”” constant=”” along=”” the=”” dipole,=”” as=”” was=”” done=”” in=”” section=”” 9-1,=”” a=”” more=”” realistic=”” approximation=”” that=”” insures=”” that=”” the=”” current=”” goes=”” to=”” zero=”” at=”” the=”” ends=”” is=”” to=”” describe=”” i=”” (z)=”” by=”” the=”” triangular=”” function=””>

As shown in Fig. 9-36 (P9.13). Use this current distribution to determine
(a) The far-field E (R, ????),
(b) The power density S (R, ????)
(c) The directivity D, and
(d) The radiation resistance Rrad.

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