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SOLUTION OF BASIC EQUATIONS OF ELECTRODYNAMICS                          185

            A circular loop antenna shown in Figure 4.3.3a is considered being electrically small if its
            diameter 2 < /30 (i.e. its circumference L < /10). The circular, square, triangle or elliptical
            loops are often used in portable mainly receiving communication systems and as a sensor for
                                                                    in the loop is set up by
            the EM fields intensity measurement. The RF conductivity current  
            the RF generator with the displayed polarity and direction at some moment of time. Due to the
            short loop circumference we can assume that the current magnitude over the loop is uniform.
            Meanwhile, some phase variation of current ∆ =  = (2 )( 10) = 0.628 [rad] aka 36°
                                                                 ⁄
                                                            ⁄
            can be expected. As a matter of fact, such short phase delay does not alter noticeably the far-
            field radiation  and can be neglected. Taking into account that the currents are oppositely
            directed along the parallel dipoles (see Figure 4.3.3b) their radiated fields are completely
            canceled in z-direction. Therefore, the vanishingly small loop has a sharp and deep radiation
            null in the direction normal to its plane. That is why loop antennas of a variety of forms are
            broadly used in radio direction finding systems. The precise line-of-direction to the source of
            radiation can be found by simple rotation of the loop shown in Figure 4.3.4a  and its pattern in
                                                                         7
            Figure 4.3.4b until the received by the loop signal reaches its minimum (along the z-axis).
            Another application is to null out one of strong uninvited or jamming signal coming to a receiver
            from some direction different from the main.

            The rigorous analysis of a circle loop radiation is cumbersome and required the acquaintance
            with the integral presentation of Bessel functions. To overcome it and simplify the far-field
            analysis let us replace the circle with inscribed square as shown in Figure 4.3.3a. We preferred
            the inscribed square to external one because of smaller error in the circumference: 11% for
            inscribed and 27% for outer. A quick look at Figure 4.3.3b reveals that the fields radiated by


                                                              Rectangular Loop






                                                                         Z




                          a)                            b)      X


                    Figure 4.3.4 a) RF amplifier connected to loop antenna, b) Radiation pattern

            square loop antenna may be viewed as the superposition of fields radiated by four electric
            dipoles located in XY-plane. The two of them, say  1  and  3 , are oriented along their -axis
            while the two others, say  2  and  4 , are perpendicular and oriented along the -axis.  Let us
            first compute the  fields emitted by the aligned dipoles  1  and  3   at  the observation point






            7  Public Domain Image, source: http://www.nationalrf.com/type_hfdf_vector.htm
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