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Lossless one-port properties; Cauer I and Foster II

Short answer

Lossless (LC) functions are odd/even or even/odd ratios with all poles and zeros simple on the jω axis alternating, positive residues, and a pole or zero at origin and infinity. For Z(s)=s(s²+4)/((s²+2)(s²+6)): Cauer I yields shunt 1F, series 0.25H, shunt 4F, series 0.0833H. Foster II yields shunt 1F, shunt 0.333H, and series LC branch 1H with 0.25F.

What are the properties of lossless one port function? Realize the following function using Cauer I and Foster II method. Z(s) = s(s²+4)/((s²+2)(s²+6))

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).

Given Z(s)=s(s2+4)(s2+2)(s2+6)=s3+4ss4+8s2+12Z(s) = \dfrac{s(s^2+4)}{(s^2+2)(s^2+6)} = \dfrac{s^3+4s}{s^4+8s^2+12}: z 0, p 1.414, z 2, p 2.449, z ∞ — alternating, odd/even, so it is a valid LC function.

Cauer-I realization

Z(s)Z(s) has a zero at s=∞s=\infty, so Y(s)=1/Z(s)Y(s)=1/Z(s) has a pole at infinity and the first element is a shunt capacitor. Divide repeatedly with polynomials in descending powers (continued fraction about s=∞s=\infty), inverting the remainder each time:

  1. Y1(s)=s4+8s2+12s3+4sY_1(s) = \frac{s^{4} + 8 s^{2} + 12}{s^{3} + 4 s} → quotient ss gives shunt C1C_1 = 1 F; remainder 4(s2+3)s(s2+4)\frac{4 \left(s^{2} + 3\right)}{s \left(s^{2} + 4\right)}.
  2. Z2(s)=s3+4s4s2+12Z_2(s) = \frac{s^{3} + 4 s}{4 s^{2} + 12} → quotient s4\frac{s}{4} gives series L2L_2 = 1/4 H (≈ 0.25 H); remainder s4(s2+3)\frac{s}{4 \left(s^{2} + 3\right)}.
  3. Y3(s)=4s2+12sY_3(s) = \frac{4 s^{2} + 12}{s} → quotient 4s4 s gives shunt C3C_3 = 4 F; remainder 12s\frac{12}{s}.
  4. Z4(s)=s12Z_4(s) = \frac{s}{12} → quotient s12\frac{s}{12} gives series L4L_4 = 1/12 H (≈ 0.08333 H); remainder 00.
ElementPositionValue
C1C_1shunt1 F
L2L_2series1/4 H (≈ 0.25 H)
C3C_3shunt4 F
L4L_4series1/12 H (≈ 0.08333 H)
o----+---[L2]----+---[L4]-+
     |           |        |
   [C1]        [C3]       |
     |           |        |
o----+-----------+--------+

Foster-II realization

Take Y(s)=1/Z(s)=s4+8s2+12s3+4sY(s) = 1/Z(s) = \frac{s^{4} + 8 s^{2} + 12}{s^{3} + 4 s} and expand Y(s)Y(s) in partial fractions (each term is an admittance; the branches are in parallel):

k∞=[Y(s)s]s→∞=1k0=[s Y(s)]s=0=32k3=[(s2+4) Y(s)s]s2=−4=1\begin{aligned} k_\infty &= \left[\frac{Y(s)}{s}\right]_{s\to\infty} = 1 \\ k_0 &= \left[s\,Y(s)\right]_{s=0} = 3 \\ 2k_{3} &= \left[\frac{(s^2+4)\,Y(s)}{s}\right]_{s^2=-4} = 1 \end{aligned} Y(s)=s+3s+ss2+4Y(s) = s + \frac{3}{s} + \frac{s}{s^{2} + 4}
TermRuleElement value
C1C_1 (shunt, pole of YY at ∞\infty)k∞k_\infty1 F
L2L_2 (shunt, pole of YY at 0)1/k01/k_01/3 H (≈ 0.3333 H)
L3L_3–C3C_3 in series (ω2=4\omega^2=4)L=1/2kL=1/2k, C=2k/ω2C=2k/\omega^2L3L_3 = 1 H, C3C_3 = 1/4 F (≈ 0.25 F)
o--+-------+-------+
   |       |       |
  [C1]    [L2]    [L3]
   |       |      [C3]
   |       |       |
o--+-------+-------+

✓ Answer checked by Claude Sonnet 5.5

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