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Filter definition and denormalization from ωold to ωnew

Short answer

A filter is a frequency-selective two-port network. Normalization uses ωo=1 rad/s and R=1 Ω for universal tables and simpler design; denormalization scales to desired frequency and impedance. To change frequency from ωold to ωnew, set kf = ωnew/ωold; then Rnew = Rold, Lnew = Lold/kf, Cnew = Cold/kf. With impedance scaling km: Rnew = km·Rold, Lnew = (km/kf)·Lold, Cnew = Cold/(km·kf).

What is Filter? Explain the significance of normalization and denormalization during filter design. Derive the expression to calculate the new values of elements that will change the operating frequency of a low pass filter from ωold to ωnew.

Filter

A filter is a frequency-selective two-port network that passes signals in a chosen band of frequencies (passband) with little attenuation and attenuates signals at other frequencies (stopband).

Significance of normalization and denormalization

Normalization means designing the filter with convenient reference values, usually a cut-off (or half-power) frequency of ωo=1\omega_o = 1 rad/s and a termination of R=1 ΩR = 1\ \Omega. Denormalization (scaling) converts the normalized element values to the actual frequency and impedance level required.

Importance:

  • Filter tables (Butterworth, Chebyshev, Bessel poles and ladder element values) are published only in normalized form; one table serves every frequency and impedance level.
  • Calculations use simple numbers like 1, 1.414, 2 instead of values like 10−910^{-9} and 10410^{4}, so errors are fewer.
  • Designs can be compared and reused: a 1 rad/s prototype becomes a 1 kHz or 1 MHz filter by simple scaling.
  • Scaling lets the designer choose practical element values (e.g. capacitors in nF–μF, resistors in kΩ) without changing the shape of the response.

New element values for changing ωold\omega_{old} to ωnew\omega_{new}

Let kf=ωnew/ωoldk_f = \omega_{new}/\omega_{old}. For the same response at the new frequency, each element's reactance at ωnew\omega_{new} must equal its old reactance at ωold\omega_{old}:

ωnewLnew=ωoldLold⇒Lnew=Loldkf1ωnewCnew=1ωoldCold⇒Cnew=ColdkfRnew=Rold\begin{aligned} \omega_{new} L_{new} = \omega_{old} L_{old} &\Rightarrow L_{new} = \frac{L_{old}}{k_f} \\ \frac{1}{\omega_{new} C_{new}} = \frac{1}{\omega_{old} C_{old}} &\Rightarrow C_{new} = \frac{C_{old}}{k_f} \\ R_{new} &= R_{old} \end{aligned}

The transfer function becomes Tnew(s)=Told(s/kf)T_{new}(s) = T_{old}(s/k_f). Combined with impedance scaling by kmk_m: R′=kmRR' = k_m R, L′=kmL/kfL' = k_m L/k_f, C′=C/(kmkf)C' = C/(k_m k_f).

Example: the normalized third-order Butterworth ladder (1 Ω, 1 H, 2 F, 1 H, 1 Ω, ωo\omega_o = 1 rad/s) scaled to ωo=104\omega_o = 10^4 rad/s (kf=104k_f = 10^4) and 1 kΩ terminations (km=1000k_m = 1000) gives RR = 1 kΩ, L=1×1000/104=0.1L = 1\times1000/10^4 = 0.1 H and C=2/(1000×104)=0.2 μC = 2/(1000\times10^4) = 0.2\ \muF.

✓ Answer checked by Claude Sonnet 5.5

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