Having difficulty in understanding how dynamic braking works while using 3 phase AC traction motors.
First, it is understood that three phase power is generated by the main traction alternator. This three phase power is then rectified (converted) to direct current (DC) by using diodes. The DC is then passed onto the inverter (consisting of either Gate Turn Off (GTO) thyristors or consisting of Insulated Gate Biplor Transistors (IGBT’s)). By adjusting the firing/switching on sequence of the inverter, the DC is then converted back to three phase power for the AC traction motors.
The AC traction motors are usually three phase asynchronous type with “squirrel cage” rotor which has large conductive metal bars instead of windings. The rotor is electrically isolated from the AC traction motor stator, and the stator consists of heavy gauge wire windings. Three phase power from the inverter is applied to the stator windings only.
Now for dynamic braking, it is understood that dynamic braking resistors are still used to dissipate heat/energy in a similar fashion to that used for DC traction motor dynamic braking.
From some diagrams seen so far on the internet, it seems the AC traction motor dynamic braking resistors are connected on the DC portion of the traction circuits between the rectifier diodes and the inverter.
It is understood that to slow the AC traction motor while in dynamic braking mode, the frequency of pulses supplied by the inverter to the AC traction motor is slower than the “mechanical frequency” of rotor rotation due to train momentum turning the wheels and then turning the traction motor rotor. The rotor tries to follow the slower electromagnetic pulse from the inverter, and this causes the rotor to resist the momentum and then creates braking.
But what is the purpose of the dynamic resistor then? With consideration of where the resistors are placed (between diodes and inverter), it seems that all they do is dissipate the DC