Well, that was not so easy! (I am not a big expert, but I have to continue, because I got involved.)The notation of your data is unconventional. I have to make some guesses. It seems reasonable to assume that:
Ra = armature resistance
La = armature (leakage) inductance
Lm = magnetization inductance
But R1, R2, L2 ?
R1 might be a starting resistance.
(Please correct me, if necessary)
R2, L2 cannot be rotor resistance and inductance, because they are zero. But because they are zero, they can be neglected (!?).
But that means that the rotor data is not given. When the rotor data is not given, the conventional guess is that the rotor resistance and inductance (as seen from the stator side) are the same as the stator resistance and inductance.
Rr' = Ra and Lr' = La
The instructions for the induction motor in ATP and ATPdraw are confusing. I have found the following to work well with the universal motor 3 model (UM3):
General:
stator coupling Y
Pole pairs 1
Rotor coils d:1 q:1
Magnet:
LMUD = LMUQ = Lm (put the magnetization inductance here)
Stator:
R(0) = 0
R(d) = R(q) = Ra ( put the stator resistance here)
L(0) = 0
L(d) = L(q) = La (put the stator inductance here, in H)
Rotor:
Use same values as for the stator
That is, do not care about the Park's transformation !
By the way, the induction motor is a tricky component in ATP. There must be some component between a source and the induction motor. A switch or a small impedance can be used.
If there are several motors in the same network, there must be a piece of transmission line connecting the motors to the network. The delay of the line must be longer than the time step, so that the line (in a way) isolates the motors from the network.
You can download a simple ATPdraw example of a network with an indcution motor at
Your data has been used in the model, but note, the rotating speed is constant.