Heidi
Member
You rather have the polarity backwards. You could say that application of a secondary current load causes an incremental reduction in the core magnetic flux. This causes an incremental reduction in the primary back EMF, causing the primary current to increase until the flux level is back up to the required value to give a back EMF equal to the primary voltage.
Sorry, I should have made the current reference directions clear at the first place.
I have found another problem, my English ablibity. I'm not sure if I understand your description. I'm not sure if I have used the terms mutual-induced, self-induced EMFs, or back EMF correctly as you do. So please allow me to start over again, and please check if I get the correct concept.
For the circuit attached, lst's focus on the time period where the voltage source v1 is increasing from zero.
One thing is for sure, that is, i1 is increasing, i2 is also increasing but in the opposite direction to the secondary current reference direction, correct?
Based on
v1(t) = L1*(di1/dt) + M*(di2/dt)
Assuming L1 and M are positive, since (di2/dt) is now negative, v1(t) is fixed at the moment, the current i1 must be increading more rapidly to make the whole term [ L1*(di1/dt) + M*(di2/dt) ] be equal v1(t).
More rapid increase in i1 means v1(t) has to increase in order to overcome the 'Back EMF' due to the increasing i1.
Do I understand you correctly?
Thank you!
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