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Lossless one-port properties; Foster I and Cauer I

Short answer

LC one-port: even/odd polynomial ratio, all poles/zeros on jω axis, simple, alternating, pole/zero at 0 and ∞, positive residues. Foster I: series L=0.5 H, C=1 F, parallel tank L=1/6 H, C=4 F. Cauer I: series 0.5 H, shunt 0.8 F, series 4.167 H, shunt 0.2 F.

What are the properties of lossless one port network circuit? The driving point impedance of one port LC network is: Z(s) = (s⁴ + 4s² + 3)/(2s³ + 3s). Obtain Foster I and Cauer I.

Properties of lossless (LC) one-port

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).

Checking the given function

Z(s)=s4+4s2+32s3+3s=(s2+1)(s2+3)2s(s2+1.5)Z(s) = \frac{s^4+4s^2+3}{2s^3+3s} = \frac{(s^2+1)(s^2+3)}{2s(s^2+1.5)}

Even/odd; poles at ω=0, 1.225, ∞\omega = 0,\ 1.225,\ \infty; zeros at ω=1, 1.732\omega = 1,\ 1.732 — they alternate (p 0, z 1, p 1.225, z 1.732, p ∞), so it is a valid LC impedance.

Foster-I form

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

k∞=[Z(s)s]s→∞=12k0=[s Z(s)]s=0=12k3=[(s2+32) Z(s)s]s2=−32=14\begin{aligned} k_\infty &= \left[\frac{Z(s)}{s}\right]_{s\to\infty} = \frac{1}{2} \\ k_0 &= \left[s\,Z(s)\right]_{s=0} = 1 \\ 2k_{3} &= \left[\frac{(s^2+\frac{3}{2})\,Z(s)}{s}\right]_{s^2=-\frac{3}{2}} = \frac{1}{4} \end{aligned} Z(s)=s2+1s+s4(s2+32)Z(s) = \frac{s}{2} + \frac{1}{s} + \frac{s}{4 \left(s^{2} + \frac{3}{2}\right)}
TermRuleElement value
L1L_1 (series, pole at ∞\infty)k∞k_\infty1/2 H (≈ 0.5 H)
C2C_2 (series, pole at 0)1/k01/k_01 F
L3∥C3L_3 \parallel C_3 (tank, ω2=32\omega^2=\frac{3}{2})C=1/2kC=1/2k, L=2k/ω2L=2k/\omega^2C3C_3 = 4 F, L3L_3 = 1/6 H (≈ 0.1667 H)
o--[L1]--[C2]--[L3||C3]--o

Cauer-I form

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)=s4+4s2+32s3+3sZ_1(s) = \frac{s^{4} + 4 s^{2} + 3}{2 s^{3} + 3 s} → quotient s2\frac{s}{2} gives series L1L_1 = 1/2 H (≈ 0.5 H); remainder 5s2+62s(2s2+3)\frac{5 s^{2} + 6}{2 s \left(2 s^{2} + 3\right)}.
  2. Y2(s)=4s3+6s5s2+6Y_2(s) = \frac{4 s^{3} + 6 s}{5 s^{2} + 6} → quotient 4s5\frac{4 s}{5} gives shunt C2C_2 = 4/5 F (≈ 0.8 F); remainder 6s5(5s2+6)\frac{6 s}{5 \left(5 s^{2} + 6\right)}.
  3. Z3(s)=25s2+306sZ_3(s) = \frac{25 s^{2} + 30}{6 s} → quotient 25s6\frac{25 s}{6} gives series L3L_3 = 25/6 H (≈ 4.167 H); remainder 5s\frac{5}{s}.
  4. Y4(s)=s5Y_4(s) = \frac{s}{5} → quotient s5\frac{s}{5} gives shunt C4C_4 = 1/5 F (≈ 0.2 F); remainder 00.
ElementPositionValue
L1L_1series1/2 H (≈ 0.5 H)
C2C_2shunt4/5 F (≈ 0.8 F)
L3L_3series25/6 H (≈ 4.167 H)
C4C_4shunt1/5 F (≈ 0.2 F)
o--[L1]----+---[L3]----+
           |           |
         [C2]        [C4]
           |           |
o----------+-----------+

✓ Answer checked by Claude Sonnet 5.5

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