Next: Finite Impulse Response Filters
Up: Clutter Rejection Filters
Previous: Clutter Rejection Filters
  Contents
Calculation of time-variant Magnitude Responses
Before start of introducing clutter rejection filters, a common
way of calculating the frequency response of a non-causal
time-variant filter is described.
A general 1-D filter operation can be expressed by a matrix
multiplication A with an input vector
=
. The input vector is an
N-dimensional complex vector
. Therefore,
the output vector y is also complex of type
. Mathematically it can be written as:
 |
(4.1) |
where A is an
matrix, and the output vector
y =
has dimension
M. With the matrix elements in row n and
k denoted by a(n,k), the elements of the output
vector are given by:
 |
(4.2) |
The filter is linear, but generally not time invariant. Therefore,
it is not possible to define the frequency response as the Fourier
transform of the impulse response
[BTK02a]. However, for a general linear
filter, the frequency response can be defined as the power of the
output signal when the input is a complex harmonic signal with
unit amplitude. As an input function, a discrete-time complex
exponential function, defined by
 |
(4.3) |
where
is the normalized angular frequency
and
is the imaginary unit can be used. With the input signal
of Eq. 4.3 the output signal becomes
 |
(4.4) |
where
is the Fourier transform of row
n in
. The frequency response then becomes
 |
(4.5) |
This general method allows the calculation of the magnitude
response of every linear time-variant non-causal filter.
Next: Finite Impulse Response Filters
Up: Clutter Rejection Filters
Previous: Clutter Rejection Filters
  Contents
Gernot Hoebenreich
2002-11-20