Principles of Planar Near-Field Antenna Measurements

Following Reference 1, consider the following testing integral
| (D.1) | |
Integrating this yields
| (D.2) | |
Thus the exact function can be expressed as
| (D.3) | |
This was evaluated numerically using the conventional discrete Fourier transform (DFT) and fast Fourier transform (FFT) and then with the trapezoidal transforms, where
| (D.4) | |
| (D.5) | |
| (D.6) | |
| (D.7) | |
| (D.8) | |
| (D.9) | |
Here, N - 1 = 80 and M = 256. The DFT was evaluated as
| (D.10) | |
The FFT was evaluated as
| (D.11) | |
Some FFTs adopt the opposite sign convention. The trapezoidal DFT was evaluated as
| (D.12) | |
Either the DFT or FFT algorithm can be employed herein. Furthermore
| (D.13) | |
| (D.14) | |
In practice, the slope of the function is obtained by central differencing, whilst a right difference is taken at the left-hand side and a left difference is taken at the right-hand side, this can be expressed explicitly as follows
| (D.15) | |
| (D.16) | |
| (D.17) | |
Results obtained from the DFT and the trapezoidal transforms can be found compared with the exact result in Figures D.1 and D.2.
Clearly, the first-order trapezoidal DFT offers a significant improvement over the more commonly employed zero-order rectangular DFT. A further comparison is made below in Table D.1. These values differ from those presented in the reference.
| m | Exact | DFT | FFT | Trapezoidal | ||||
|---|---|---|---|---|---|---|---|---|
| Mag | Arg | Mag | Arg | Mag | Arg | Mag | Arg | |
| dB |