Bilinear transform - Definition

In digital signal processing, the bilinear transform is a conformal mapping, often used to convert a transfer function <math> H_a(s) \ <math> of a linear, time-invariant (LTI) filter in the continuous-time domain (often called an analog filter) to a transfer function <math> H_d(z) \ <math> of a linear, shift-invariant filter in the discrete-time domain (often called a digital filter although there are analog filters constructed with charge-coupled devices that are discrete-time filters). It maps positions on the <math> j \omega \ <math> axis, <math> Re[s]=0 \ <math> , in the s-plane to the unit circle, <math> |z| = 1 \ <math>, in the z-plane . Other bilinear transforms can be used to warp the frequency response of any discrete-time linear system (e.g., to approximate the human auditory's non-linear frequency resolution) and are implementable in the discrete domain by replacing a system's unit delays <math> \left( z^{-1} \right) \ <math> with first order all-pass filters.

The transform preserves stability and maps every point of the frequency response of the continuous-time filter, <math> H_a(j \omega_a) \ <math> to a corresponding point in the frequency response of the discrete-time filter, <math> H_d(e^{j \omega_d T}) \ <math> although to a somewhat different frequency, as shown in the Frequency Warping section below. This means that for every feature that one sees in the frequency response of the analog filter, there is a corresponding feature, with identical gain and phase shift, in the frequency response of the digital filter but, perhaps, at a somewhat different frequency. This is barely noticeable at low frequencies but is quite evident at frequencies close to the Nyquist frequency.

The bilinear transform is a first-order approximation of the natural logarithm function that is an exact mapping of the z-plane to the s-plane. When the Laplace transform of a discrete-time signal (with each element of the discrete-time sequence attached to an appropriately delayed unit impulse), the result is precisely the Z transform of the discrete-time sequence with the substitution of

<math>z \ <math>	<math> = e^{sT} \ <math>
	<math> = \frac{e^{sT/2}}{e^{-sT/2}} \ <math>
	<math> \approx \frac{1 + s T / 2}{1 - s T / 2} \ <math>

where <math> T \ <math> is the sample time (the reciprocal of the sampling frequency) of the discrete-time filter. The above bilinear approximation can be solved for <math> s \ <math> or a similar approximation for <math> s = (1/T) \log(z) \ \ <math> can be performed.

The inverse of this mapping (and its first-order bilinear approximation) is

<math>s \ <math>	<math> = \frac{1}{T} \log(z) \ <math>
	<math> = \frac{2}{T} \left[ \frac{z-1}{z+1} + \frac{1}{3} \left( \frac{z-1}{z+1} \right)^3 + \frac{1}{5} \left( \frac{z-1}{z+1} \right)^5 + \frac{1}{7} \left( \frac{z-1}{z+1} \right)^7 + \ldots \right] \ <math>
	<math> \approx \frac{2}{T} \frac{z - 1}{z + 1} \ <math>

<math>s \leftarrow \frac{2}{T} \frac{z - 1}{z + 1}<math>

That is

<math>H_d(z) = H_a(s) \bigg|_{s = \frac{2}{T} \frac{z - 1}{z + 1}}= H_a \left( \frac{2}{T} \frac{z-1}{z+1} \right) \ <math>

The bilinear transform is a special case of a conformal mapping, namely, the Möbius transformation defined as

<math>z^{\prime} = \frac{a z + b}{c z + d}.<math>

Background

A continuous-time filter is stable if the poles of its transfer function fall in the negative real half of the complex s-plane. A discrete-time filter is stable if the poles of its transfer function fall inside the unit circle in the complex z-plane. The bilinear transform maps the negative real half of the complex s-plane to the interior of the unit circle in the z-plane. Thus filters designed in the continuous-time domain that are stable are converted to filters the discrete-time domain that preserve that stability.

Example

As an example take a simple RC-filter. This continuous-time filter has a transfer function

<math>H_a(s) = \frac{1}{1 + RC s}<math>

If we wish to implement this filter as a digital filter, we can apply the bilinear transform by substituting for <math>s<math> the formula above; after some reworking, we get the following filter representation:

<math>H_d(z) \ <math>	<math> =H_a \left( \frac{2}{T} \frac{z-1}{z+1}\right) \ <math>
	<math>= \frac{1}{1 + RC \left( \frac{2}{T} \frac{z-1}{z+1}\right)} \ <math>
	<math>= \frac{1 + z}{(1 - 2 RC / T) + (1 + 2RC / T) z} \ <math>

Frequency warping

To determine the frequency response of a contiuous-time filter, the transfer function <math> H_a(s) \ <math> is evaluated at <math>s = j \omega \ <math> which is on the <math> j \omega \ <math> axis. Likewise, to determine the frequency response of a discrete-time filter, the transfer function <math> H_d(z) \ <math> is evaluated at <math>z = e^{ j \omega T} \ <math> which is on the unit circle, <math> |z| = 1 \ <math>. When the actual frequency of <math> \omega_d \ <math> is input to the discrete-time filter designed by use of the bilinear transform, it is desired to know at what frequency, <math> \omega_a \ <math>, for the continuous-time filter that this <math> \omega_d \ <math> is mapped to.

<math>H_d(z) = H_a \left( \frac{2}{T} \frac{z-1}{z+1}\right) \ <math>

<math>H_d(e^{ j \omega T}) \ <math>	<math>= H_a \left( \frac{2}{T} \frac{e^{ j \omega T} - 1}{e^{ j \omega T} + 1}\right) \ <math>
	<math>= H_a \left( \frac{2}{T} \cdot \frac{e^{j \omega_d T/2} \left(e^{j \omega_d T/2} - e^{-j \omega_d T/2}\right)}{e^{j \omega_d T/2} \left(e^{j \omega_d T/2} + e^{-j \omega_d T/2 }\right)}\right) \ <math>
	<math>= H_a \left( \frac{2}{T} \cdot \frac{\left(e^{j \omega_d T/2} - e^{-j \omega_d T/2}\right)}{\left(e^{j \omega_d T/2} + e^{-j \omega_d T/2 }\right)}\right) \ <math>
	<math>= H_a \left(j \frac{2}{T} \cdot \frac{ \left(e^{j \omega_d T/2} - e^{-j \omega_d T/2}\right) /(2j)}{\left(e^{j \omega_d T/2} + e^{-j \omega_d T/2 }\right) / 2}\right) \ <math>
	<math>= H_a \left(j \frac{2}{T} \cdot \frac{ \sin(\omega_d T/2) }{ \cos(\omega_d T/2) }\right) \ <math>
	<math>= H_a \left(j \frac{2}{T} \cdot \tan \left( \omega_d \frac{T}{2} \right) \right) \ <math>
	<math>= H_a \left(j \omega_a \right) \ <math>

<math> \omega_a = \frac{2}{T} \tan \left( \omega_d \frac{T}{2} \right) <math>

and the inverse mapping is

<math> \omega_d = \frac{2}{T} \arctan \left( \omega_a \frac{T}{2} \right) <math>.

The discrete-time filter behaves at frequency <math>\omega \ <math> the same way that the continuous-time filter behaves at frequency <math> (2/T) \tan(\omega T/2) \ <math>. Specifically, the gain and phase shift that the discrete-time filter has at frequency <math>\omega \ <math> the same gain and phase shift that the continuous-time filter has at frequency <math> (2/T) \tan(\omega T/2) \ <math>.

One can see that the entire continuous frequency range

<math> -\infty \leq \omega_a \leq +\infty <math>

is mapped onto the fundamental frequency interval

<math> -\frac{\pi}{T} \leq \omega_d \leq +\frac{\pi}{T}.<math>

The continuous-time filter frequency <math> \omega_a = 0 \ <math> corresponds to the discrete-time filter frequency <math> \omega_d = 0 \ <math> and the continuous-time filter frequency <math> \omega_a = \pm \infty \ <math> correspond to the discrete-time filter frequency <math> \omega_d = \pm \pi / T \ <math>.

One can also see that there is a nonlinear relationship between <math> \omega_a \ <math> and <math> \omega_d \ <math>. This effect of the bilinear transform is called frequency warping.

The main advantage of the warping phenomenon is the absence of aliasing distortion of the frequency response characteristic, such as observed with the impulse invariant method. It is necessary, however, to compensate for the frequency warping by pre-warping the given frequency specifications of the continuous-time system. These pre-warped specifications may then be used in the bilinear transform to obtain the desired discrete-time system.