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Validate LC impedance; Foster I and Cauer II

Short answer

Factor Z(s)=8s(s²+1.25)/((s²+1)(s²+5)). It's odd/even; poles at ω=1,√5 and zeros at 0,√1.25,∞ alternate with zeros at 0 and ∞, residues positive → valid LC. Foster I: series L₁=0.5H∥C₁=2F, L₂=1.5H∥C₂≈0.133F. Cauer II: shunt 2H, series 0.2F, shunt 1.5H, series 1/3F.

How can you assure that the following function is a valid LC impedance function? Z(s) = (8s³+10s)/(5+6s²+s⁴). Synthesize it using Foster I and Cauer II form.

Checking validity

A given Z(s)Z(s) is checked as follows:

  1. Factor numerator and denominator. Each must be a product of factors ss and (s2+ωi2)(s^2+\omega_i^2) only, so that one is even and the other odd.
  2. Write the critical frequencies in increasing order of ω\omega and check that poles and zeros alternate.
  3. Check that there is a pole or zero at s=0s=0 and at s=∞s=\infty (degrees differ by exactly 1).
  4. Check that all residues of the partial-fraction expansion are positive (this follows when steps 1–3 hold).

For the given function:

Z(s)=8s3+10ss4+6s2+5=8s(s2+1.25)(s2+1)(s2+5)Z(s) = \frac{8s^3+10s}{s^4+6s^2+5} = \frac{8s(s^2+1.25)}{(s^2+1)(s^2+5)}

Odd/even; zeros at ω=0, 1.118, ∞\omega = 0,\ 1.118,\ \infty (degree 3 over 4), poles at ω=1, 2.236\omega = 1,\ 2.236; order z 0, p 1, z 1.118, p 2.236, z ∞ — they alternate, with a zero at both s=0s=0 and s=∞s=\infty. Valid LC impedance. The partial fractions below also give positive residues, which confirms it.

Foster-I form

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

2k1=[(s2+1) Z(s)s]s2=−1=122k2=[(s2+5) Z(s)s]s2=−5=152\begin{aligned} 2k_{1} &= \left[\frac{(s^2+1)\,Z(s)}{s}\right]_{s^2=-1} = \frac{1}{2} \\ 2k_{2} &= \left[\frac{(s^2+5)\,Z(s)}{s}\right]_{s^2=-5} = \frac{15}{2} \end{aligned} Z(s)=s2(s2+1)+15s2(s2+5)Z(s) = \frac{s}{2 \left(s^{2} + 1\right)} + \frac{15 s}{2 \left(s^{2} + 5\right)}
TermRuleElement value
L1∥C1L_1 \parallel C_1 (tank, ω2=1\omega^2=1)C=1/2kC=1/2k, L=2k/ω2L=2k/\omega^2C1C_1 = 2 F, L1L_1 = 1/2 H (≈ 0.5 H)
L2∥C2L_2 \parallel C_2 (tank, ω2=5\omega^2=5)C=1/2kC=1/2k, L=2k/ω2L=2k/\omega^2C2C_2 = 2/15 F (≈ 0.1333 F), L2L_2 = 3/2 H (≈ 1.5 H)
o--[L1||C1]--[L2||C2]--o

Cauer-II form

Z(s)Z(s) has a zero at s=0s=0, so Y(s)=1/Z(s)Y(s)=1/Z(s) has a pole at the origin and the first element is a shunt inductor. 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. Y1(s)=5+6s2+s410s+8s3Y_1(s) = \frac{5 + 6 s^{2} + s^{4}}{10 s + 8 s^{3}} → quotient 12s\frac{1}{2 s} gives shunt L1L_1 = 2 H; remainder s(s2+2)2(4s2+5)\frac{s \left(s^{2} + 2\right)}{2 \left(4 s^{2} + 5\right)}.
  2. Z2(s)=10+8s22s+s3Z_2(s) = \frac{10 + 8 s^{2}}{2 s + s^{3}} → quotient 5s\frac{5}{s} gives series C2C_2 = 1/5 F (≈ 0.2 F); remainder 3ss2+2\frac{3 s}{s^{2} + 2}.
  3. Y3(s)=2+s23sY_3(s) = \frac{2 + s^{2}}{3 s} → quotient 23s\frac{2}{3 s} gives shunt L3L_3 = 3/2 H (≈ 1.5 H); remainder s3\frac{s}{3}.
  4. Z4(s)=3sZ_4(s) = \frac{3}{s} → quotient 3s\frac{3}{s} gives series C4C_4 = 1/3 F (≈ 0.3333 F); remainder 00.
ElementPositionValue
L1L_1shunt2 H
C2C_2series1/5 F (≈ 0.2 F)
L3L_3shunt3/2 H (≈ 1.5 H)
C4C_4series1/3 F (≈ 0.3333 F)
o----+---[C2]----+---[C4]-+
     |           |        |
   [L1]        [L3]       |
     |           |        |
o----+-----------+--------+

✓ Answer checked by Claude Sonnet 5.5

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