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Valid lossless function; Foster II and Cauer II

Short answer

Valid lossless: (ii) Z(s)=(s⁴+4s²+3)/(s(s²+2)); poles/zeros on jω axis alternate, pole at 0, pole at ∞. Foster II: parallel branches: series L=2 H, C=0.5 F; series L=2 H, C=1/6 F. Cauer II: series 2/3 F, shunt 1.25 H, series 0.08 F, shunt 5 H.

Which of the following is valid lossless function? State with reason. Pick one of the valid LC lossless functions and synthesize it using Foster II and Cauer II methods. (i) Z(s) = (s²+4)(s²+5)/((s²+2)(s²+10)) (ii) Z(s) = (s⁴+4s²+3)/(s(s²+2)) (iii) Z(s) = (s⁶+4s⁴+8s²)/(s³+3s)

Checking the functions

Tests for a valid LC impedance: (1) even/odd or odd/even ratio, (2) simple poles and zeros only on the jωj\omega axis, (3) poles and zeros alternate, (4) a pole or a zero at both s=0s=0 and s=∞s=\infty (degrees differ by exactly 1), (5) positive residues.

FunctionFactored form / critical frequenciesResult
(i) (s2+4)(s2+5)(s2+2)(s2+10)\dfrac{(s^2+4)(s^2+5)}{(s^2+2)(s^2+10)}p 1.414, z 2, z 2.236, p 3.162Even/even with equal degrees (no pole/zero at 00, ∞\infty); zeros adjacent → invalid
(ii) s4+4s2+3s(s2+2)=(s2+1)(s2+3)s(s2+2)\dfrac{s^4+4s^2+3}{s(s^2+2)} = \dfrac{(s^2+1)(s^2+3)}{s(s^2+2)}p 0, z 1, p 1.414, z 1.732, p ∞Even/odd, alternate → valid
(iii) s6+4s4+8s2s3+3s=s(s4+4s2+8)s2+3\dfrac{s^6+4s^4+8s^2}{s^3+3s} = \dfrac{s(s^4+4s^2+8)}{s^2+3}s4+4s2+8=0s^4+4s^2+8=0 gives s2=−2±j2s^2=-2\pm j2Zeros are complex (not on jωj\omega axis); degrees differ by 3 → invalid

Function (ii) is synthesized.

Foster-II form

Take Y(s)=1/Z(s)=s3+2ss4+4s2+3Y(s) = 1/Z(s) = \frac{s^{3} + 2 s}{s^{4} + 4 s^{2} + 3} and expand Y(s)Y(s) in partial fractions (each term is an admittance; the branches are in parallel):

2k1=[(s2+1) Y(s)s]s2=−1=122k2=[(s2+3) Y(s)s]s2=−3=12\begin{aligned} 2k_{1} &= \left[\frac{(s^2+1)\,Y(s)}{s}\right]_{s^2=-1} = \frac{1}{2} \\ 2k_{2} &= \left[\frac{(s^2+3)\,Y(s)}{s}\right]_{s^2=-3} = \frac{1}{2} \end{aligned} Y(s)=s2(s2+1)+s2(s2+3)Y(s) = \frac{s}{2 \left(s^{2} + 1\right)} + \frac{s}{2 \left(s^{2} + 3\right)}
TermRuleElement value
L1L_1–C1C_1 in series (ω2=1\omega^2=1)L=1/2kL=1/2k, C=2k/ω2C=2k/\omega^2L1L_1 = 2 H, C1C_1 = 1/2 F (≈ 0.5 F)
L2L_2–C2C_2 in series (ω2=3\omega^2=3)L=1/2kL=1/2k, C=2k/ω2C=2k/\omega^2L2L_2 = 2 H, C2C_2 = 1/6 F (≈ 0.1667 F)
o--+-------+
   |       |
  [L1]    [L2]
  [C1]    [C2]
   |       |
o--+-------+

Cauer-II form

Z(s)Z(s) has a pole at s=0s=0, so the first element is a series capacitor. Arrange numerator and denominator in ascending powers of ss and divide repeatedly (continued fraction about s=0s=0); each quotient is k/sk/s:

  1. Z1(s)=3+4s2+s42s+s3Z_1(s) = \frac{3 + 4 s^{2} + s^{4}}{2 s + s^{3}} → quotient 32s\frac{3}{2 s} gives series C1C_1 = 2/3 F (≈ 0.6667 F); remainder s(2s2+5)2(s2+2)\frac{s \left(2 s^{2} + 5\right)}{2 \left(s^{2} + 2\right)}.
  2. Y2(s)=4+2s25s+2s3Y_2(s) = \frac{4 + 2 s^{2}}{5 s + 2 s^{3}} → quotient 45s\frac{4}{5 s} gives shunt L2L_2 = 5/4 H (≈ 1.25 H); remainder 2s5(2s2+5)\frac{2 s}{5 \left(2 s^{2} + 5\right)}.
  3. Z3(s)=25+10s22sZ_3(s) = \frac{25 + 10 s^{2}}{2 s} → quotient 252s\frac{25}{2 s} gives series C3C_3 = 2/25 F (≈ 0.08 F); remainder 5s5 s.
  4. Y4(s)=15sY_4(s) = \frac{1}{5 s} → quotient 15s\frac{1}{5 s} gives shunt L4L_4 = 5 H; remainder 00.
ElementPositionValue
C1C_1series2/3 F (≈ 0.6667 F)
L2L_2shunt5/4 H (≈ 1.25 H)
C3C_3series2/25 F (≈ 0.08 F)
L4L_4shunt5 H
o--[C1]----+---[C3]----+
           |           |
         [L2]        [L4]
           |           |
o----------+-----------+

✓ Answer checked by Claude Sonnet 5.5

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