IEEE Circuits and Systems Magazine - Q2 2018 - 22

Im p1(V ), Im p2 (V )

4

L∗ = 41.67 mH

V = -7 V
Re p1 = 0
Im p1 = 2.4495
V = -6.95 V

2
V = -7.1 V
V = -4.9 V
V = -8.1 V
-8

-6

V = -8.7 V
-4

V = -5 V

V = -0.55 V

V = 8.7 V

-2

Re p1(V ),
Re p2 (V )

0
V = 8.7 V

V = -8.7 V

V = -8.1 V

V = -0.55 V

V = -5 V

V = -4.9 V
-2
V = -6.95 V

V = -7.1 V

V = -7 V
Re p2 = 0
Im p2 = -2.4495

-4
(a)
Im p1(L ), Im p2 (L )

V = -7 V

4

L = L∗ = 41.67 mH
Re p1 = 0
Im p1 = 2.4495

L = 40.67 mH

L = 42.67 mH
2

L = 95 mH

L = 10 µH
L = 18.8 mH
-∞

0

-5

5
L=∞

L = 18.8 mH

L=0

L = 453.03 mH
L=∞

L=0

Re p1(L ),
Re p2 (L )

L = 95 mH
L = 453.03 mH

L = 10 µH
-2

L = 42.67 mH
L = 40.67 mH
-4

L = L∗ = 41.67 mH
Re p2 = 0
Im p2 = -2.4495

(b)
Figure 8. (a). loci of the real and imaginary parts of poles of YC (s, V) where the input voltage V is a parameter and the inductance
L = L * = 41.67 mH. (b). loci of the real and imaginary parts of poles of YC (s, V) where the external inductance l is a parameter
and the voltage V = - 7 V.

22

IEEE cIrcuIts and systEms magazInE

sEcOnd quartEr 2018



Table of Contents for the Digital Edition of IEEE Circuits and Systems Magazine - Q2 2018

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