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Zeros of transmission and their realization

Short answer

Zeros of transmission are s-values where the transfer function is zero. In an LC ladder they come from a series arm becoming an open circuit or a shunt arm a short circuit. Zeros at 0 and ∞ result from complete pole removal; finite zeros need zero shifting. e.g., a series capacitor yields a zero at s=0, a shunt series-LC branch yields a finite zero at 1/√(LC).

What are zeros of transmission (in a two port network)? How can zeros of transmission be realized in a network? Explain with suitable examples.

Zeros of transmission of a two-port network are the values of complex frequency ss at which the transfer function (z21z_{21}, y21y_{21}, V2/V1V_2/V_1 or I2/I1I_2/I_1) is zero, i.e. a finite input produces no output at that frequency. For an LC ladder they lie on the jωj\omega axis (including s=0s=0 and s=∞s=\infty).

Realization of transmission zeros

In a ladder, a signal is blocked when a series arm is an open circuit (its impedance has a pole) or a shunt arm is a short circuit (its impedance has a zero, i.e. its admittance has a pole). So the transmission zeros of a ladder are the poles of the series-arm impedances and the poles of the shunt-arm admittances.

Element / armTransmission zero at
Series LLs=∞s=\infty (open at high frequency)
Shunt CCs=∞s=\infty (short at high frequency)
Series CCs=0s=0 (open at dc)
Shunt LLs=0s=0 (short at dc)
Series arm: L∥CL \parallel C tankω=1/LC\omega = 1/\sqrt{LC} (tank impedance → ∞)
Shunt arm: LL–CC in seriesω=1/LC\omega = 1/\sqrt{LC} (branch impedance → 0)
 zero at w1=1/sqrt(L1C1)   zero at w2=1/sqrt(L2C2)
o--[L1||C1]--+---------o
             |
            [L2]
            [C2]
             |
o------------+---------o

Zeros at 00 and ∞\infty are obtained by complete removal of poles of ZZ or YY at 00 or ∞\infty (Cauer-type steps). A zero at a finite frequency ωz\omega_z is obtained by zero shifting (partial pole removal) followed by complete removal of the pole at ±jωz\pm j\omega_z.

Example. Realize Z(s)=(s2+1)(s2+3)s(s2+2)Z(s) = \dfrac{(s^2+1)(s^2+3)}{s(s^2+2)} as a ladder with a transmission zero at ω=2\omega = 2 rad/s.

The zeros of ZZ are at ω=1\omega = 1 and 1.7321.732; we need one at ω=2\omega=2, so remove part of the pole at ∞\infty: Z1(s)=Z(s)−ksZ_1(s) = Z(s) - k s with Z1(j2)=0Z_1(j2) = 0.

Z(j2)=(−4+1)(−4+3)j2(−4+2)=3−j4=j0.75Z1(j2)=j0.75−j2k=0  ⇒  k=38Z1(s)=Z(s)−38s=(s2+4)(5s2+6)8s(s2+2)\begin{aligned} Z(j2) &= \frac{(-4+1)(-4+3)}{j2(-4+2)} = \frac{3}{-j4} = j0.75 \\ Z_1(j2) &= j0.75 - j2k = 0 \;\Rightarrow\; k = \tfrac{3}{8} \\ Z_1(s) &= Z(s) - \tfrac{3}{8}s = \frac{(s^2+4)(5s^2+6)}{8s(s^2+2)} \end{aligned}

So series L1=3/8L_1 = 3/8 H, and Z1Z_1 now has a zero at s=±j2s=\pm j2 (the other zero moved from 1 to 1.095 rad/s). Its reciprocal has a pole at ±j2\pm j2, removed completely as a shunt branch:

Y1(s)=8s(s2+2)(s2+4)(5s2+6)=87ss2+4+16s7(5s2+6)87ss2+4⇒L2=78 H, C2=27 F(1/L2C2=2)Z2(s)=7(5s2+6)16s=3516s+218s⇒L3=3516 H, C3=821 F\begin{aligned} Y_1(s) &= \frac{8s(s^2+2)}{(s^2+4)(5s^2+6)} = \frac{\tfrac{8}{7}s}{s^2+4} + \frac{16s}{7(5s^2+6)} \\ \tfrac{8}{7}\tfrac{s}{s^2+4} &\Rightarrow L_2 = \tfrac{7}{8}\ \text{H},\ C_2 = \tfrac{2}{7}\ \text{F}\quad (1/\sqrt{L_2C_2} = 2) \\ Z_2(s) &= \frac{7(5s^2+6)}{16s} = \tfrac{35}{16}s + \frac{21}{8s} \Rightarrow L_3 = \tfrac{35}{16}\ \text{H},\ C_3 = \tfrac{8}{21}\ \text{F} \end{aligned}
o--[L1=3/8H]--+--[L3=35/16H]--[C3=8/21F]--+
              |                           |
          [L2=7/8H]                       |
          [C2=2/7F]                       |
              |                           |
o-------------+---------------------------+

The shunt branch L2L_2–C2C_2 shorts the signal at ω=2\omega=2 rad/s, which is the required transmission zero. (Check: rebuilding the ladder gives back the original Z(s)Z(s).)

✓ Answer checked by Claude Sonnet 5.5

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