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LC impedance check; Foster parallel and Cauer I

Short answer

Valid: Z(s)=(s⁴+10s²+9)/(s³+4s) because poles/zeros on jω axis alternate, odd/even, positive residues. The other has adjacent poles and negative residue. Foster parallel: two series-LC branches in parallel: 8/3H with 3/8F, and 8/5H with 5/72F. Cauer I: series 1H, shunt 1/6F, series 2.4H, shunt 0.2778F.

Which of the following functions are LC driving point impedance function and why? Z(s) = (s⁴+10s²+9)/(s³+4s); Z(s) = (s³+4s)/(s⁴+5s²+6). Also find the Foster parallel and cauer I form of the valid LC driving point impedance function.

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.

  • Z(s)=s4+10s2+9s3+4s=(s2+1)(s2+9)s(s2+4)Z(s) = \dfrac{s^4+10s^2+9}{s^3+4s} = \dfrac{(s^2+1)(s^2+9)}{s(s^2+4)}: p 0, z 1, p 2, z 3, p ∞ — alternate. Valid LC.
  • Z(s)=s3+4ss4+5s2+6=s(s2+4)(s2+2)(s2+3)Z(s) = \dfrac{s^3+4s}{s^4+5s^2+6} = \dfrac{s(s^2+4)}{(s^2+2)(s^2+3)}: z 0, p 1.414, p 1.732, z 2 — two poles adjacent; the residue at s2=−3s^2=-3 is [s2+4s2+2]s2=−3=1−1=−1<0\left[\frac{s^2+4}{s^2+2}\right]_{s^2=-3} = \frac{1}{-1} = -1 < 0. Not LC.

Foster parallel (Foster-II) form

Take Y(s)=1/Z(s)=s3+4ss4+10s2+9Y(s) = 1/Z(s) = \frac{s^{3} + 4 s}{s^{4} + 10 s^{2} + 9} and expand Y(s)Y(s) in partial fractions (each term is an admittance; the branches are in parallel):

2k1=[(s2+1) Y(s)s]s2=−1=382k2=[(s2+9) Y(s)s]s2=−9=58\begin{aligned} 2k_{1} &= \left[\frac{(s^2+1)\,Y(s)}{s}\right]_{s^2=-1} = \frac{3}{8} \\ 2k_{2} &= \left[\frac{(s^2+9)\,Y(s)}{s}\right]_{s^2=-9} = \frac{5}{8} \end{aligned} Y(s)=3s8(s2+1)+5s8(s2+9)Y(s) = \frac{3 s}{8 \left(s^{2} + 1\right)} + \frac{5 s}{8 \left(s^{2} + 9\right)}
TermRuleElement value
L1L_1–C1C_1 in series (ω2=1\omega^2=1)L=1/2kL=1/2k, C=2k/ω2C=2k/\omega^2L1L_1 = 8/3 H (≈ 2.667 H), C1C_1 = 3/8 F (≈ 0.375 F)
L2L_2–C2C_2 in series (ω2=9\omega^2=9)L=1/2kL=1/2k, C=2k/ω2C=2k/\omega^2L2L_2 = 8/5 H (≈ 1.6 H), C2C_2 = 5/72 F (≈ 0.06944 F)
o--+-------+
   |       |
  [L1]    [L2]
  [C1]    [C2]
   |       |
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+10s2+9s3+4sZ_1(s) = \frac{s^{4} + 10 s^{2} + 9}{s^{3} + 4 s} → quotient ss gives series L1L_1 = 1 H; remainder 3(2s2+3)s(s2+4)\frac{3 \left(2 s^{2} + 3\right)}{s \left(s^{2} + 4\right)}.
  2. Y2(s)=s3+4s6s2+9Y_2(s) = \frac{s^{3} + 4 s}{6 s^{2} + 9} → quotient s6\frac{s}{6} gives shunt C2C_2 = 1/6 F (≈ 0.1667 F); remainder 5s6(2s2+3)\frac{5 s}{6 \left(2 s^{2} + 3\right)}.
  3. Z3(s)=12s2+185sZ_3(s) = \frac{12 s^{2} + 18}{5 s} → quotient 12s5\frac{12 s}{5} gives series L3L_3 = 12/5 H (≈ 2.4 H); remainder 185s\frac{18}{5 s}.
  4. Y4(s)=5s18Y_4(s) = \frac{5 s}{18} → quotient 5s18\frac{5 s}{18} gives shunt C4C_4 = 5/18 F (≈ 0.2778 F); remainder 00.
ElementPositionValue
L1L_1series1 H
C2C_2shunt1/6 F (≈ 0.1667 F)
L3L_3series12/5 H (≈ 2.4 H)
C4C_4shunt5/18 F (≈ 0.2778 F)
o--[L1]----+---[L3]----+
           |           |
         [C2]        [C4]
           |           |
o----------+-----------+

✓ Answer checked by Claude Sonnet 5.5

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