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Lossless check; Cauer-I and Foster-I expansions

Short answer

Only Z(s)=(s⁵+10s³+24s)/(s⁴+6s²+5) is lossless: poles/zeros on jω axis, alternating, zero at 0, pole at ∞. Cauer I: series 1 H, shunt 0.25 F, series 3.2 H, shunt 5/12 F, series 0.6 H. Foster I: series 1 H, parallel tank (15/4 H, 4/15 F), parallel tank (1/20 H, 4 F).

Which of the following function is lossless and why? Find the Cauer-I and Foster-I expansion for the corresponding lossless function. Z(s) = (s² + 10s + 24)/(s² + 8s + 15); Z(s) = (s⁵ + 10s³ + 24s)/(s⁴ + 6s² + 5)

Which function is lossless

  • Z(s)=s2+10s+24s2+8s+15=(s+4)(s+6)(s+3)(s+5)Z(s) = \dfrac{s^2+10s+24}{s^2+8s+15} = \dfrac{(s+4)(s+6)}{(s+3)(s+5)}: numerator and denominator contain both odd and even powers (not an even/odd ratio); poles and zeros lie on the negative real axis, not the jωj\omega axis; there is no pole or zero at 00 or ∞\infty. Not lossless (it has the form of an RC impedance: p 3, z 4, p 5, z 6).
  • Z(s)=s5+10s3+24ss4+6s2+5=s(s2+4)(s2+6)(s2+1)(s2+5)Z(s) = \dfrac{s^5+10s^3+24s}{s^4+6s^2+5} = \dfrac{s(s^2+4)(s^2+6)}{(s^2+1)(s^2+5)}: odd/even; zeros at ω=0,2,2.449\omega = 0, 2, 2.449, poles at ω=1,2.236,∞\omega = 1, 2.236, \infty; order z 0, p 1, z 2, p 2.236, z 2.449, p ∞ — they alternate. Valid lossless (LC) function.

Cauer-I expansion

Z(s)Z(s) has a pole at s=∞s=\infty (numerator degree is higher), so the first element is a series inductor. Divide repeatedly with polynomials in descending powers (continued fraction about s=∞s=\infty), inverting the remainder each time:

  1. Z1(s)=s5+10s3+24ss4+6s2+5Z_1(s) = \frac{s^{5} + 10 s^{3} + 24 s}{s^{4} + 6 s^{2} + 5} → quotient ss gives series L1L_1 = 1 H; remainder s(4s2+19)(s2+1)(s2+5)\frac{s \left(4 s^{2} + 19\right)}{\left(s^{2} + 1\right) \left(s^{2} + 5\right)}.
  2. Y2(s)=s4+6s2+54s3+19sY_2(s) = \frac{s^{4} + 6 s^{2} + 5}{4 s^{3} + 19 s} → quotient s4\frac{s}{4} gives shunt C2C_2 = 1/4 F (≈ 0.25 F); remainder 5(s2+4)4s(4s2+19)\frac{5 \left(s^{2} + 4\right)}{4 s \left(4 s^{2} + 19\right)}.
  3. Z3(s)=16s3+76s5s2+20Z_3(s) = \frac{16 s^{3} + 76 s}{5 s^{2} + 20} → quotient 16s5\frac{16 s}{5} gives series L3L_3 = 16/5 H (≈ 3.2 H); remainder 12s5(s2+4)\frac{12 s}{5 \left(s^{2} + 4\right)}.
  4. Y4(s)=5s2+2012sY_4(s) = \frac{5 s^{2} + 20}{12 s} → quotient 5s12\frac{5 s}{12} gives shunt C4C_4 = 5/12 F (≈ 0.4167 F); remainder 53s\frac{5}{3 s}.
  5. Z5(s)=3s5Z_5(s) = \frac{3 s}{5} → quotient 3s5\frac{3 s}{5} gives series L5L_5 = 3/5 H (≈ 0.6 H); remainder 00.
ElementPositionValue
L1L_1series1 H
C2C_2shunt1/4 F (≈ 0.25 F)
L3L_3series16/5 H (≈ 3.2 H)
C4C_4shunt5/12 F (≈ 0.4167 F)
L5L_5series3/5 H (≈ 0.6 H)
o--[L1]----+---[L3]----+---[L5]-+
           |           |        |
         [C2]        [C4]       |
           |           |        |
o----------+-----------+--------+

Foster-I expansion

Expand Z(s)Z(s) in partial fractions (each term is an impedance; the elements are in series):

k∞=[Z(s)s]s→∞=12k2=[(s2+1) Z(s)s]s2=−1=1542k3=[(s2+5) Z(s)s]s2=−5=14\begin{aligned} k_\infty &= \left[\frac{Z(s)}{s}\right]_{s\to\infty} = 1 \\ 2k_{2} &= \left[\frac{(s^2+1)\,Z(s)}{s}\right]_{s^2=-1} = \frac{15}{4} \\ 2k_{3} &= \left[\frac{(s^2+5)\,Z(s)}{s}\right]_{s^2=-5} = \frac{1}{4} \end{aligned} Z(s)=s+15s4(s2+1)+s4(s2+5)Z(s) = s + \frac{15 s}{4 \left(s^{2} + 1\right)} + \frac{s}{4 \left(s^{2} + 5\right)}
TermRuleElement value
L1L_1 (series, pole at ∞\infty)k∞k_\infty1 H
L2∥C2L_2 \parallel C_2 (tank, ω2=1\omega^2=1)C=1/2kC=1/2k, L=2k/ω2L=2k/\omega^2C2C_2 = 4/15 F (≈ 0.2667 F), L2L_2 = 15/4 H (≈ 3.75 H)
L3∥C3L_3 \parallel C_3 (tank, ω2=5\omega^2=5)C=1/2kC=1/2k, L=2k/ω2L=2k/\omega^2C3C_3 = 4 F, L3L_3 = 1/20 H (≈ 0.05 H)
o--[L1]--[L2||C2]--[L3||C3]--o

✓ Answer checked by Claude Sonnet 5.5

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