Gain and Radiation Resistance
In absence of power losses, the power radiated by any antenna must be equal to its input power. In other words, the radiation resistance of a lossless antenna must match its input resistance. When comparing these two resistances we have another validation check of a numerical method.
Fig. 1 shows the input resistance of a center-fed cylindrical antenna of length L = 0.5 m, radius a = 5 mm and source gap g = L/200 as a function of frequency. On the other hand, the radiation resistance has been calculated as the ratio of the radiated power to the square of the absolute value of the input current at the source position.
The radiated power can be obtained from the Power Budget > window in the AN-SOF Results menu. The difference between both resistances is numerically negligible as can be seen. In Fig. 2 the percentage difference between the input and radiation resistances plotted in Fig. 1 is shown. The error is really very small, it is below 0.035%.
Regarding the antenna gain, we can investigate its convergence behavior as the number of segments is increased. In Fig. 3 the gain of a half-wave dipole versus the total number of segments along the antenna is shown. The gain values converge monotonically from 3 segments. The error between the gain values and its asymptotic value is also shown in Fig. 3. Only with 5 segments in half-wavelength, so 10 segments per wavelength, the error in the gain is less than 0.5%, which is a really low error. This is another confirmation that results with practical value can be obtained using 10 segments per wavelength.