TY - GEN
T1 - Defining the starting distance for the far field of antennas operating in any environment
AU - Abdallah, M. N.
AU - Sarkar, T. K.
AU - Monebhurrun, Vikass
AU - Salazar-Palma, M.
N1 - Publisher Copyright:
© 2016 IEEE.
PY - 2017/1/12
Y1 - 2017/1/12
N2 - The far field of an antenna is generally considered to be the region where the outgoing wavefront is planar and the antenna radiation pattern has a polar variation and is independent of the distance from the antenna. In this paper, the starting distance for the far field is defined for antennas operating in free space and over an imperfect ground plane. First, this paper intends to illustrate that 2D2 / λ formula, where D is the maximum dimension of the antenna and λ is the operating wavelength, is not universally valid, it is only valid for antennas where D >> λ. Second, this paper intends to compute a more specific constraint so instead of D >> λ we compute a threshold for D after which the 2D2 / λ formula applies. Third, this paper intends to properly interpret D in the formula 2D2 / λ when the antenna is operating over an imperfect ground plane. In this paper, we do not use 2D2 / λ for antennas operating over an imperfect ground instead we use a formula which depends on the transmitting and receiving antenna's heights over the air-Earth interface.
AB - The far field of an antenna is generally considered to be the region where the outgoing wavefront is planar and the antenna radiation pattern has a polar variation and is independent of the distance from the antenna. In this paper, the starting distance for the far field is defined for antennas operating in free space and over an imperfect ground plane. First, this paper intends to illustrate that 2D2 / λ formula, where D is the maximum dimension of the antenna and λ is the operating wavelength, is not universally valid, it is only valid for antennas where D >> λ. Second, this paper intends to compute a more specific constraint so instead of D >> λ we compute a threshold for D after which the 2D2 / λ formula applies. Third, this paper intends to properly interpret D in the formula 2D2 / λ when the antenna is operating over an imperfect ground plane. In this paper, we do not use 2D2 / λ for antennas operating over an imperfect ground instead we use a formula which depends on the transmitting and receiving antenna's heights over the air-Earth interface.
KW - Far Field
KW - Near Field
KW - Radial
KW - Transverse
UR - http://www.scopus.com/inward/record.url?scp=85013150629&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85013150629&partnerID=8YFLogxK
U2 - 10.1109/CAMA.2016.7815743
DO - 10.1109/CAMA.2016.7815743
M3 - Conference contribution
AN - SCOPUS:85013150629
T3 - 2016 IEEE Conference on Antenna Measurements and Applications, CAMA 2016
BT - 2016 IEEE Conference on Antenna Measurements and Applications, CAMA 2016
PB - Institute of Electrical and Electronics Engineers Inc.
T2 - 2016 IEEE Conference on Antenna Measurements and Applications, CAMA 2016
Y2 - 23 October 2016 through 27 October 2016
ER -