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Valid lossless function; Foster series and Cauer I

Short answer

Functions (ii) and (iii) are valid lossless. For (iii), Foster-I gives series L=2H, parallel L=3H||C=0.333F and L=0.333H||C=1F; Cauer-I gives series L=2H, shunt C=0.25F, series L=2.667H, shunt C=0.75F, series L=0.667H.

Which of the following is valid lossless function? State with reason. Pick one of the valid LC lossless functions and synthesize it using Foster series and Cauer I methods. i) Z(s) = (s²+4)(s²+5)/((s²+2)(s²+10)) ii) Z(s) = (s⁴+4s²+3)/(s(s²+2)) iii) Z(s) = (2s⁵+12s³+16s)/(s⁴+4s²+3) iv) Z(s) = (s⁶+4s⁴+8s²)/(s³+3s)

Checking 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.

FunctionFactored form / critical frequenciesResult
(i) (s2+4)(s2+5)(s2+2)(s2+10)\dfrac{(s^2+4)(s^2+5)}{(s^2+2)(s^2+10)}p 1.414, z 2, z 2.236, p 3.162Even/even, equal degrees; zeros adjacent → invalid
(ii) (s2+1)(s2+3)s(s2+2)\dfrac{(s^2+1)(s^2+3)}{s(s^2+2)}p 0, z 1, p 1.414, z 1.732, p ∞Even/odd, alternate → valid
(iii) 2s(s2+2)(s2+4)(s2+1)(s2+3)\dfrac{2s(s^2+2)(s^2+4)}{(s^2+1)(s^2+3)}z 0, p 1, z 1.414, p 1.732, z 2, p ∞Odd/even, alternate → valid
(iv) s(s4+4s2+8)s2+3\dfrac{s(s^4+4s^2+8)}{s^2+3}s4+4s2+8=0s^4+4s^2+8=0 gives s2=−2±j2s^2=-2\pm j2Complex zeros; degrees differ by 3 → invalid

Valid functions: (ii) and (iii). We synthesize (iii):

Z(s)=2s5+12s3+16ss4+4s2+3=2s(s2+2)(s2+4)(s2+1)(s2+3)Z(s) = \frac{2s^5+12s^3+16s}{s^4+4s^2+3} = \frac{2s(s^2+2)(s^2+4)}{(s^2+1)(s^2+3)}

Foster series (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→∞=22k2=[(s2+1) Z(s)s]s2=−1=32k3=[(s2+3) Z(s)s]s2=−3=1\begin{aligned} k_\infty &= \left[\frac{Z(s)}{s}\right]_{s\to\infty} = 2 \\ 2k_{2} &= \left[\frac{(s^2+1)\,Z(s)}{s}\right]_{s^2=-1} = 3 \\ 2k_{3} &= \left[\frac{(s^2+3)\,Z(s)}{s}\right]_{s^2=-3} = 1 \end{aligned} Z(s)=2s+3ss2+1+ss2+3Z(s) = 2 s + \frac{3 s}{s^{2} + 1} + \frac{s}{s^{2} + 3}
TermRuleElement value
L1L_1 (series, pole at ∞\infty)k∞k_\infty2 H
L2∥C2L_2 \parallel C_2 (tank, ω2=1\omega^2=1)C=1/2kC=1/2k, L=2k/ω2L=2k/\omega^2C2C_2 = 1/3 F (≈ 0.3333 F), L2L_2 = 3 H
L3∥C3L_3 \parallel C_3 (tank, ω2=3\omega^2=3)C=1/2kC=1/2k, L=2k/ω2L=2k/\omega^2C3C_3 = 1 F, L3L_3 = 1/3 H (≈ 0.3333 H)
o--[L1]--[L2||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)=2s5+12s3+16ss4+4s2+3Z_1(s) = \frac{2 s^{5} + 12 s^{3} + 16 s}{s^{4} + 4 s^{2} + 3} → quotient 2s2 s gives series L1L_1 = 2 H; remainder 2s(2s2+5)(s2+1)(s2+3)\frac{2 s \left(2 s^{2} + 5\right)}{\left(s^{2} + 1\right) \left(s^{2} + 3\right)}.
  2. Y2(s)=s4+4s2+34s3+10sY_2(s) = \frac{s^{4} + 4 s^{2} + 3}{4 s^{3} + 10 s} → quotient s4\frac{s}{4} gives shunt C2C_2 = 1/4 F (≈ 0.25 F); remainder 3(s2+2)4s(2s2+5)\frac{3 \left(s^{2} + 2\right)}{4 s \left(2 s^{2} + 5\right)}.
  3. Z3(s)=8s3+20s3s2+6Z_3(s) = \frac{8 s^{3} + 20 s}{3 s^{2} + 6} → quotient 8s3\frac{8 s}{3} gives series L3L_3 = 8/3 H (≈ 2.667 H); remainder 4s3(s2+2)\frac{4 s}{3 \left(s^{2} + 2\right)}.
  4. Y4(s)=3s2+64sY_4(s) = \frac{3 s^{2} + 6}{4 s} → quotient 3s4\frac{3 s}{4} gives shunt C4C_4 = 3/4 F (≈ 0.75 F); remainder 32s\frac{3}{2 s}.
  5. Z5(s)=2s3Z_5(s) = \frac{2 s}{3} → quotient 2s3\frac{2 s}{3} gives series L5L_5 = 2/3 H (≈ 0.6667 H); remainder 00.
ElementPositionValue
L1L_1series2 H
C2C_2shunt1/4 F (≈ 0.25 F)
L3L_3series8/3 H (≈ 2.667 H)
C4C_4shunt3/4 F (≈ 0.75 F)
L5L_5series2/3 H (≈ 0.6667 H)
o--[L1]----+---[L3]----+---[L5]-+
           |           |        |
         [C2]        [C4]       |
           |           |        |
o----------+-----------+--------+

✓ Answer checked by Claude Sonnet 5.5

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