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To get started with nec2 I tried to simulate a simple dipole.
The graphical view of the pattern looks okay, however the gain seems to be to high. To what are the DBs refered in the output file? [...] If I calculate the gain with the formula: 4 * Pi * r^2 * |E|^2 Gain = ----------------------- P_in * 2 * 120 * Pi by using the E-Field magnitude values from nec2's output I get also those very high values. (?) PS, also confused by your formula. Which Value of E are you using? Are you The formula should be correct: I just use the magnitude value of the E Field. The intensitiy W_rad is then 0.5 * |E|^2 / Z_w (E and H are in phase and orthogonal in the far field) The radiation density U is then r^2 * W_rad (Unit: Watt per solid angle) The radiation density U_0 of an isotropic radiator with a total radiated power P_rad is: P_rad / (4 * Pi). The gain is then U/U_0 (or in dBi: 10*log(U/U_0) ). trying to calculate the "Total radiated power" (TRP)? If so you need to integrate the power density over a spherical region. The calculation is Yes, but nec2 shows the total radiated power in its output. As for your RP card, I notice that you are attempting to vary both "Theta" and "Phi". I usually keep one fixed and vary the other, but to be honest I am not sure if what you are doing is incorrect, although I notice that the "Phi" pattern is only computed for one frequency. The only other difference No thats no true. In the output file I can see E_phi as well as E_theta for every combination of phi and theta (for every frequency). I use the programm Xnecview to view the pattern and it has problems if you don't have points over the full sphere. is that I normally do not use gain averaging. Also using 1 degree The average gain (over the full sphere) should probably be 1 (or 0 dBi). I get 0.991. Thanks for you help! The bad computation was caused by the stupid segementation I had chosen. Detlef |
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