π²The original version of my LF/MF MOSFET Class-E πΌtransmitter power amplifier design was described on π
6 December 2015, with follow-ups on π
9 January 2016 & π
21 September 2017. It has been in regular use since then. However, several modifications have been made recently.
The ➰inductive reactance of the bias choke has been increased to the approximate optimal value of 30x MOSFET drain resistance, ( see Note below ), to improve the performance on the LF π2190m/∿136KHz band. So a second ⊚T200-26 core and a ⊚T157-52 core with 29 & 18 turn windings respectively have been added in series with the original ⊚T200-26 core; all are iron powder toroidal cores.
The ➿inductor in the original LF band module could become quite hot. Two replacement modules have been made; one is completely new and uses Litz wire for the ➿inductor, while the other is a redesign of the original still using 16 gauge enamelled copper wire (ecw), but changing capacitor values by "select-on-test". The coil-former for the 'ecw' ➿inductor was 3-D printed from PETG filament, and is partially ribbed along its length. The DC blocking capacitor has to be a low-loss type as the RF current through it can be considerable. Here, I have used several capacitors connected in parallel to share the current. The spacing between the ➿inductor and ground-plane has been increased to reduce losses. Both designs for the LF band module will be tested in turn for comparison.
Currently the output power is 210 watts on MF (π»π630m/∿472KHz band ), 282 watts on LF (π» π2190m/∿136KHz band Litz wire coil in band module ) and 302 watts on LF ( π»π2190m/∿136KHz band 16-gauge ecw coil in band module ) - see image below.π³
Note: for Class E, Drain Load Resistance = (Supply Volts)π 2 / 1.2 x Output Power




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