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Lossless properties; Foster series and Cauer I

Short answer

Lossless LC: even/odd polynomial ratio, jω poles/zeros alternate, positive residues, dX/dω>0. Valid: Z=2(s⁴+9s²+8)/(s³+4s) (p0,z1,p2,z√8,p∞ alternate). Foster series: L=2H, C=0.25F, tank L=1.5H∥C≈0.167F. Cauer I: series L=2H, shunt C=0.1F, series L≈4.167H, shunt C=0.15F.

What are the properties of lossless one port function? Determine whether the following are lossless function or not? State with reason. Z(s) = 2(s⁴+9s²+8)/(s³+4s); Z(s) = (s³+s)/(s⁴+12s²+32); Z(s) = (s³+4s)/(s⁴+4s²+3). Realize one of the valid lossless function using Foster Series and cauer I methods.

Properties of lossless one-port function

An LC (lossless) driving-point immittance Z(s)Z(s) or Y(s)Y(s) has these properties:

  1. It is the ratio of an even polynomial to an odd polynomial, or odd to even, with real, positive coefficients.
  2. All poles and zeros are simple and lie on the jωj\omega axis (they occur in conjugate pairs ±jωi\pm j\omega_i).
  3. Poles and zeros alternate (interlace) along the jωj\omega axis.
  4. The highest powers of numerator and denominator differ by exactly 1; so do the lowest powers.
  5. There is always either a pole or a zero at s=0s=0, and either a pole or a zero at s=∞s=\infty.
  6. The residues at all poles are real and positive.
  7. On the jωj\omega axis Z(jω)=jX(ω)Z(j\omega)=jX(\omega) is purely reactive and dX/dω>0dX/d\omega>0 (Foster's reactance theorem).

Testing the functions

FunctionFactored formCritical frequenciesResult
Z1=2(s4+9s2+8)s3+4sZ_1 = \dfrac{2(s^4+9s^2+8)}{s^3+4s}2(s2+1)(s2+8)s(s2+4)\dfrac{2(s^2+1)(s^2+8)}{s(s^2+4)}p 0, z 1, p 2, z 2.828, p ∞Even/odd, alternate → valid
Z2=s3+ss4+12s2+32Z_2 = \dfrac{s^3+s}{s^4+12s^2+32}s(s2+1)(s2+4)(s2+8)\dfrac{s(s^2+1)}{(s^2+4)(s^2+8)}z 0, z 1, p 2, p 2.828, z ∞Zeros 0 and 1 adjacent → invalid
Z3=s3+4ss4+4s2+3Z_3 = \dfrac{s^3+4s}{s^4+4s^2+3}s(s2+4)(s2+1)(s2+3)\dfrac{s(s^2+4)}{(s^2+1)(s^2+3)}z 0, p 1, p 1.732, z 2, z ∞Poles 1 and 1.732 adjacent → invalid

Only Z1(s)=2(s2+1)(s2+8)s(s2+4)Z_1(s) = \dfrac{2(s^2+1)(s^2+8)}{s(s^2+4)} is lossless.

Foster series (Foster-I) realization

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

k∞=[Z(s)s]s→∞=2k0=[s Z(s)]s=0=42k3=[(s2+4) Z(s)s]s2=−4=6\begin{aligned} k_\infty &= \left[\frac{Z(s)}{s}\right]_{s\to\infty} = 2 \\ k_0 &= \left[s\,Z(s)\right]_{s=0} = 4 \\ 2k_{3} &= \left[\frac{(s^2+4)\,Z(s)}{s}\right]_{s^2=-4} = 6 \end{aligned} Z(s)=2s+4s+6ss2+4Z(s) = 2 s + \frac{4}{s} + \frac{6 s}{s^{2} + 4}
TermRuleElement value
L1L_1 (series, pole at ∞\infty)k∞k_\infty2 H
C2C_2 (series, pole at 0)1/k01/k_01/4 F (≈ 0.25 F)
L3∥C3L_3 \parallel C_3 (tank, ω2=4\omega^2=4)C=1/2kC=1/2k, L=2k/ω2L=2k/\omega^2C3C_3 = 1/6 F (≈ 0.1667 F), L3L_3 = 3/2 H (≈ 1.5 H)
o--[L1]--[C2]--[L3||C3]--o

Cauer-I realization

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)=2s4+18s2+16s3+4sZ_1(s) = \frac{2 s^{4} + 18 s^{2} + 16}{s^{3} + 4 s} → quotient 2s2 s gives series L1L_1 = 2 H; remainder 2(5s2+8)s(s2+4)\frac{2 \left(5 s^{2} + 8\right)}{s \left(s^{2} + 4\right)}.
  2. Y2(s)=s3+4s10s2+16Y_2(s) = \frac{s^{3} + 4 s}{10 s^{2} + 16} → quotient s10\frac{s}{10} gives shunt C2C_2 = 1/10 F (≈ 0.1 F); remainder 6s5(5s2+8)\frac{6 s}{5 \left(5 s^{2} + 8\right)}.
  3. Z3(s)=25s2+406sZ_3(s) = \frac{25 s^{2} + 40}{6 s} → quotient 25s6\frac{25 s}{6} gives series L3L_3 = 25/6 H (≈ 4.167 H); remainder 203s\frac{20}{3 s}.
  4. Y4(s)=3s20Y_4(s) = \frac{3 s}{20} → quotient 3s20\frac{3 s}{20} gives shunt C4C_4 = 3/20 F (≈ 0.15 F); remainder 00.
ElementPositionValue
L1L_1series2 H
C2C_2shunt1/10 F (≈ 0.1 F)
L3L_3series25/6 H (≈ 4.167 H)
C4C_4shunt3/20 F (≈ 0.15 F)
o--[L1]----+---[L3]----+
           |           |
         [C2]        [C4]
           |           |
o----------+-----------+

✓ Answer checked by Claude Sonnet 5.5

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