Let us connect a sinusoidal voltage source of value, E as shown in Fig. 2. Let Iˉ1 and Iˉ2 be the mesh currents.
Now, Equivalent inductive reactance, jωLeq=I1E
Let us name the coils as shown in Fig. 2. Now, I1 is the current through coil-A, I1−I2 is the current through coil-B and I2 is the current through coils C and D.
The current flowing in each coupled coil will induce an emf in the other coil. Therefore, in the circuit of Fig. 2, there will be four mutual induced emfs as explained below :
Emf-1: The current Iˉ1 entering at the undotted end in coil-A will induce an emf j2ωIˉ1 in coil-C such that the undotted end is positive.
Emf-2 : The current Iˉ1−Iˉ2 entering at the dotted end in coil-B will induce an emf j3ω(I1−I2) in coil-D such that the dotted end is positive.
Emf-3 : The current Iˉ2 entering at the dotted end in coil-C will induce an emf j2ωIˉ2 in coil-A such that the dotted end is positive.
Emf-4: The current I2 entering at the dotted end in coil-D will induce an emf j3ωI2 in coil-B such that the dotted end is positive.
The self- and mutual induced emfs in the coils are shown in Fig. 3.
By KVL in mesh-1,
j5ωI1+j6ω(I1−I2)+j3ωI2=j2ωI2+E∴j11ωI1−j5ωI2=E …..(1)
By KVL in mesh-2,
j8ωI2+j9ωI2+j3ω(I1−I2)=j6ω(I1−I2)+j3ωI2+j2ωI1∴−j5ωI1+j17ωI2=0 …..(2)
On arranging equations (1) and (2) in matrix form we get,
[j11ω–j5ω–j5ωj17ω][I1I2]=[E0]
Now, Δ1=∣∣∣∣∣Eˉ0−j5ωj17ω∣∣∣∣∣=Eˉ×j17ω−0=j17ωEˉ
Δ=∣∣∣∣∣j11ω−j5ω−j5ωj17ω∣∣∣∣∣=j11ω×j17ω−(−j5ω)2=−187ω2+25ω2=−162ω2
I1=ΔΔ1=−162ω2j17ωE=j162ω17E∴I1E=17j162ω
Here, Iˉ1Eˉ=jωLeq ,∴jωLeq =17j162ω⇒Leq =17162H
RESULT
Equivalent inductance, Leq=17162H=9.5294H