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LC impedance check; Foster-I and Cauer-I

Short answer

Only Z3(s) = 2(s²+1)(s²+9)/(s(s²+4)) is valid: it has an odd/even ratio, simple alternating jω poles/zeros (p0,z1,p2,z3,p∞), and degrees differ by 1. Foster I yields series L1=2 H, C2=2/9 F, parallel tank L3=15/8 H, C3=2/15 F. Cauer I gives L1=2 H, shunt C2=1/12 F, series L3=24/5 H, shunt C4=5/36 F.

Which of the following functions are LC driving point impedance function and why? Pick one of the valid LC driving point impedance and synthesize it in Foster-I and Cauer-I form: Z1(s) = (s²+1)(s²+5)/((s²+2)(s²+10)); Z2(s) = 5s(s²+4)/((s²+1)(s²+3)); Z3(s) = 2(s²+1)(s²+9)/(s(s²+4)); Z4(s) = 4(s+2)(s+5)/((s+1)(s+4))

Testing the functions

Tests for a valid LC impedance: (1) even/odd or odd/even ratio, (2) simple poles and zeros only on the jωj\omega axis, (3) poles and zeros alternate, (4) a pole or a zero at both s=0s=0 and s=∞s=\infty (degrees differ by exactly 1), (5) positive residues.

FunctionCritical frequenciesResult
Z1=(s2+1)(s2+5)(s2+2)(s2+10)Z_1 = \dfrac{(s^2+1)(s^2+5)}{(s^2+2)(s^2+10)}z 1, p 1.414, z 2.236, p 3.162Even/even, equal degrees: no pole or zero at 00 and ∞\infty → invalid
Z2=5s(s2+4)(s2+1)(s2+3)Z_2 = \dfrac{5s(s^2+4)}{(s^2+1)(s^2+3)}z 0, p 1, p 1.732, z 2Adjacent poles → invalid
Z3=2(s2+1)(s2+9)s(s2+4)Z_3 = \dfrac{2(s^2+1)(s^2+9)}{s(s^2+4)}p 0, z 1, p 2, z 3, p ∞Even/odd, alternate → valid
Z4=4(s+2)(s+5)(s+1)(s+4)Z_4 = \dfrac{4(s+2)(s+5)}{(s+1)(s+4)}negative real axisRC type, not LC → invalid

Synthesize Z3(s)=2s4+20s2+18s3+4sZ_3(s) = \dfrac{2s^4+20s^2+18}{s^3+4s}.

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→∞=2k0=[s Z(s)]s=0=922k3=[(s2+4) Z(s)s]s2=−4=152\begin{aligned} k_\infty &= \left[\frac{Z(s)}{s}\right]_{s\to\infty} = 2 \\ k_0 &= \left[s\,Z(s)\right]_{s=0} = \frac{9}{2} \\ 2k_{3} &= \left[\frac{(s^2+4)\,Z(s)}{s}\right]_{s^2=-4} = \frac{15}{2} \end{aligned} Z(s)=2s+92s+15s2(s2+4)Z(s) = 2 s + \frac{9}{2 s} + \frac{15 s}{2 \left(s^{2} + 4\right)}
TermRuleElement value
L1L_1 (series, pole at ∞\infty)k∞k_\infty2 H
C2C_2 (series, pole at 0)1/k01/k_02/9 F (≈ 0.2222 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 = 2/15 F (≈ 0.1333 F), L3L_3 = 15/8 H (≈ 1.875 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)=2s4+20s2+18s3+4sZ_1(s) = \frac{2 s^{4} + 20 s^{2} + 18}{s^{3} + 4 s} → quotient 2s2 s gives series L1L_1 = 2 H; remainder 6(2s2+3)s(s2+4)\frac{6 \left(2 s^{2} + 3\right)}{s \left(s^{2} + 4\right)}.
  2. Y2(s)=s3+4s12s2+18Y_2(s) = \frac{s^{3} + 4 s}{12 s^{2} + 18} → quotient s12\frac{s}{12} gives shunt C2C_2 = 1/12 F (≈ 0.08333 F); remainder 5s12(2s2+3)\frac{5 s}{12 \left(2 s^{2} + 3\right)}.
  3. Z3(s)=24s2+365sZ_3(s) = \frac{24 s^{2} + 36}{5 s} → quotient 24s5\frac{24 s}{5} gives series L3L_3 = 24/5 H (≈ 4.8 H); remainder 365s\frac{36}{5 s}.
  4. Y4(s)=5s36Y_4(s) = \frac{5 s}{36} → quotient 5s36\frac{5 s}{36} gives shunt C4C_4 = 5/36 F (≈ 0.1389 F); remainder 00.
ElementPositionValue
L1L_1series2 H
C2C_2shunt1/12 F (≈ 0.08333 F)
L3L_3series24/5 H (≈ 4.8 H)
C4C_4shunt5/36 F (≈ 0.1389 F)
o--[L1]----+---[L3]----+
           |           |
         [C2]        [C4]
           |           |
o----------+-----------+

✓ Answer checked by Claude Sonnet 5.5

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