rezna
Newbie level 6
Hi
I have only one "free to use" article which is related with Wu-king Theory (I hope it is free, because you can find it and download it from internet there: https://users.ece.gatech.edu/~wrscott/).
Other sources are not free (IEEE,..) sorry
However, Wu-King dipole is easy to describe. It is every (for example dipole structure) with this resistive loading along dipole (from port to the end of structure):
Z(x)=(60*Psi)/(h-x) where "x" is position along dipole, "h" is length of dipole, and Psi is:
Psi = 2*[1/(sinh(h/a)-C(2A,2kh)-j*S(2A,2kh)]+1/(kh)*(1-exp(-j2kh)) (it is for dipole structure where "a" is radius of this dipole)
C(2A,2kh) and S(2A,2kh) are generalized cosine and sine integrals.
I have only one "free to use" article which is related with Wu-king Theory (I hope it is free, because you can find it and download it from internet there: https://users.ece.gatech.edu/~wrscott/).
Other sources are not free (IEEE,..) sorry
However, Wu-King dipole is easy to describe. It is every (for example dipole structure) with this resistive loading along dipole (from port to the end of structure):
Z(x)=(60*Psi)/(h-x) where "x" is position along dipole, "h" is length of dipole, and Psi is:
Psi = 2*[1/(sinh(h/a)-C(2A,2kh)-j*S(2A,2kh)]+1/(kh)*(1-exp(-j2kh)) (it is for dipole structure where "a" is radius of this dipole)
C(2A,2kh) and S(2A,2kh) are generalized cosine and sine integrals.