For part B, you have R4 = 200 ohms from part 1?
So Z4 = 200+jwl, easily solved with l = 510mH, w = 6.28e3
Z3 = 100 +jwl with l being 250mH in this case.
Now form two potential dividers Z3/(Z3+R1) and Z4/(Z4+R2)
The offset voltage is simply 5 * ((Z3/(Z3+R1)) - (Z4/(Z4+R2))).
Now the answer will be a voltage phasor in the complex plane, something of the form a+jb volts, the in phase component is simply a volts and the quadrature component is simply b volts, the unit vector ~j being at rightangles the the natural numbers, no need for trig here unless you did the algenbra in polar coordinates.
I leave the algebra to you.
Note that you will need to label which side of the bridge is positive to make the answer complete.
Regards, Dan.
BTW The easy way yo analyse that bridge in balance is to imagine applying DC where it becomes obvious that as R2 is twice R1, R4 must be twice R3, the same reasoning them applies to the inductors to keep the ratios the same.
Regards, Dan.