High-frequency resistance p.u.l. of a coaxial cable. Assume that the coaxial cable in Fig.9.2 has small conductor losses. From Eqs.(9.7), the complex rms magnetic field intensities on surfaces of the inner (r = a+) and outer (r = b−) conductors of the
cable are , respectively. The vector H is entirely tangential to both surfaces, so that the integral in Eqs.(9.12) results in the following expression for the high-frequency resistance per unit length of the cable:
Write a function resistanceCoaxCable() in MATLAB that calculates R_.
Reference: Equation
Reference: Figure
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