Wilkinson power divider is an N-port passive device [1], however it is commonly found as a 2-way divider (3 ports). By manipulating the S-parameter matrix, it can be shown that it is unfeasible to achieve a 3-port device that it is at the same time:
A Wilkinson power divider is a device that is matched at all ports, lossless when excited in the input port and the output ports are kept isolated. Its S-Parameter matrix for equal power division is given by Eq. 1) and its basic layout is shown in Fig. 2. In order to fully analyze this structure, one can use an "odd-even analysis" and for a complete treatment of it, please refer to [2]
Fig. 2 shows a schematic of a Wilkinson divider that can easily be constructed in CST STUDIO SUITE® (Fig. 3). Full dimensions are provided in the model construction notes. The model is simulated with the time domain solver in the frequency range 0 to 2 GHz.
| Parameter | Value | Description |
| h | Substrate thickness | |
| eps_r | Substrate permitivity | |
| t | Metallization thickness | |
| W50 | 50 |
|
| W70 | ||
| l70 | Length of |
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In Fig. 1 we see the E-field animation when the port 1 (input) is excited. The input signal flows through the split and is divided in ports 2 and 3. Fig. 4 shows the E-field animation when port 2 is excited. Note that the signal flows through the split, but practically nothing is coupled to port 3.
The S-parameters results are shown in Fig. 5. Note that ports 1, 2 and 3 are matched.
The equal power distribution can be seen by the overlapping curves of
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