< 8:31 Antennas Past papers Sessional-II.pdf Quaid-i-Azam University Sessional-II, Spring 2021 (Antennas (EL-724) 50% Date: 17-06-2021 NOTE: Due date for submission of Sessional-II is 17-06-2021 at 4:30 pm. Question 1 Consider a linear wire antenna of finite length and radius a. The radius a of the antenna is taken to be very small as compared to an operating wavelength A, i.e., a << A. The electric current density vector J(r) of the antenna is given by, J(r) =ė, 16()()() f(h's) = sink(1/2 h)] sin kl/2] - where h, and hy are dummy coordinates which form a three perpendicular coordinate system and 5(-) is a Dirac delta function. The geometry of the problem is given in Fig. 1. It should be noted that here axial unit vector è, in spherical coordinates are given below, =è, sine, coso, +ê, sin 0, sino, + è, cose, Find the electric and magnetic fields in the near and far zone. Also find the maximum directivity D- ← а
< 8:31 Antennas Past papers Sessional-II.pdf Quaid-i-Azam University Sessional-II, Spring 2021 (Antennas (EL-724) 50% Date: 17-06-2021 NOTE: Due date for submission of Sessional-II is 17-06-2021 at 4:30 pm. Question 1 Consider a linear wire antenna of finite length and radius a. The radius a of the antenna is taken to be very small as compared to an operating wavelength A, i.e., a << A. The electric current density vector J(r) of the antenna is given by, J(r) =ė, 16()()() f(h's) = sink(1/2 h)] sin kl/2] - where h, and hy are dummy coordinates which form a three perpendicular coordinate system and 5(-) is a Dirac delta function. The geometry of the problem is given in Fig. 1. It should be noted that here axial unit vector è, in spherical coordinates are given below, =è, sine, coso, +ê, sin 0, sino, + è, cose, Find the electric and magnetic fields in the near and far zone. Also find the maximum directivity D- ← а
Introductory Circuit Analysis (13th Edition)
13th Edition
ISBN:9780133923605
Author:Robert L. Boylestad
Publisher:Robert L. Boylestad
Chapter1: Introduction
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