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Transform 1-D FIR Filter to 2-D FIR Filter |
For information about designing linear filters in the spatial domain, see What Is Image Filtering in the Spatial Domain?.
This example shows how to transform a one-dimensional FIR filter into a two-dimensional FIR filter using the ftrans2 function. This function can be useful because it is easier to design a one-dimensional filter with particular characteristics than a corresponding two-dimensional filter. The frequency transformation method preserves most of the characteristics of the one-dimensional filter, particularly the transition bandwidth and ripple characteristics. The shape of the one-dimensional frequency response is clearly evident in the two-dimensional response.
This function uses atransformation matrix, a set of elements that defines the frequency transformation. This function's default transformation matrix produces filters with nearly circular symmetry. By defining your own transformation matrix, you can obtain different symmetries. (See Jae S. Lim, Two-Dimensional Signal and Image Processing, 1990, for details.)
Create 1-D FIR filter.
b = remez(10,[0 0.4 0.6 1],[1 1 0 0])
b = Columns 1 through 9 0.0537 -0.0000 -0.0916 -0.0001 0.3131 0.4999 0.3131 -0.0001 -0.0916 Columns 10 through 11 -0.0000 0.0537
Transform the 1-D filter to a 2-D filter.
h = ftrans2(b);
h = Columns 1 through 9 0.0001 0.0005 0.0024 0.0063 0.0110 0.0132 0.0110 0.0063 0.0024 0.0005 0.0031 0.0068 0.0042 -0.0074 -0.0147 -0.0074 0.0042 0.0068 0.0024 0.0068 -0.0001 -0.0191 -0.0251 -0.0213 -0.0251 -0.0191 -0.0001 0.0063 0.0042 -0.0191 -0.0172 0.0128 0.0259 0.0128 -0.0172 -0.0191 0.0110 -0.0074 -0.0251 0.0128 0.0924 0.1457 0.0924 0.0128 -0.0251 0.0132 -0.0147 -0.0213 0.0259 0.1457 0.2021 0.1457 0.0259 -0.0213 0.0110 -0.0074 -0.0251 0.0128 0.0924 0.1457 0.0924 0.0128 -0.0251 0.0063 0.0042 -0.0191 -0.0172 0.0128 0.0259 0.0128 -0.0172 -0.0191 0.0024 0.0068 -0.0001 -0.0191 -0.0251 -0.0213 -0.0251 -0.0191 -0.0001 0.0005 0.0031 0.0068 0.0042 -0.0074 -0.0147 -0.0074 0.0042 0.0068 0.0001 0.0005 0.0024 0.0063 0.0110 0.0132 0.0110 0.0063 0.0024 Columns 10 through 11 0.0005 0.0001 0.0031 0.0005 0.0068 0.0024 0.0042 0.0063 -0.0074 0.0110 -0.0147 0.0132 -0.0074 0.0110 0.0042 0.0063 0.0068 0.0024 0.0031 0.0005 0.0005 0.0001
View the frequency response of the filters.
[H,w] = freqz(b,1,64,'whole');
colormap(jet(64))
plot(w/pi-1,fftshift(abs(H)))
figure, freqz2(h,[32 32])
One-Dimensional Frequency Response
Corresponding Two-Dimensional Frequency Response
The frequency sampling method creates a filter based on a desired frequency response. Given a matrix of points that define the shape of the frequency response, this method creates a filter whose frequency response passes through those points. Frequency sampling places no constraints on the behavior of the frequency response between the given points; usually, the response ripples in these areas. (Ripples are oscillations around a constant value. The frequency response of a practical filter often has ripples where the frequency response of an ideal filter is flat.)
The toolbox function fsamp2 implements frequency sampling design for two-dimensional FIR filters. fsamp2 returns a filter h with a frequency response that passes through the points in the input matrix Hd. The example below creates an 11-by-11 filter using fsamp2 and plots the frequency response of the resulting filter. (The freqz2 function in this example calculates the two-dimensional frequency response of a filter. See Computing the Frequency Response of a Filter for more information.)
Hd = zeros(11,11); Hd(4:8,4:8) = 1; [f1,f2] = freqspace(11,'meshgrid'); mesh(f1,f2,Hd), axis([-1 1 -1 1 0 1.2]), colormap(jet(64)) h = fsamp2(Hd); figure, freqz2(h,[32 32]), axis([-1 1 -1 1 0 1.2])
Desired Two-Dimensional Frequency Response (left) and Actual Two-Dimensional Frequency Response (right)
Notice the ripples in the actual frequency response, compared to the desired frequency response. These ripples are a fundamental problem with the frequency sampling design method. They occur wherever there are sharp transitions in the desired response.
You can reduce the spatial extent of the ripples by using a larger filter. However, a larger filter does not reduce the height of the ripples, and requires more computation time for filtering. To achieve a smoother approximation to the desired frequency response, consider using the frequency transformation method or the windowing method.
The windowing method involves multiplying the ideal impulse response with a window function to generate a corresponding filter, which tapers the ideal impulse response. Like the frequency sampling method, the windowing method produces a filter whose frequency response approximates a desired frequency response. The windowing method, however, tends to produce better results than the frequency sampling method.
The toolbox provides two functions for window-based filter design, fwind1 and fwind2. fwind1 designs a two-dimensional filter by using a two-dimensional window that it creates from one or two one-dimensional windows that you specify. fwind2 designs a two-dimensional filter by using a specified two-dimensional window directly.
fwind1 supports two different methods for making the two-dimensional windows it uses:
Transforming a single one-dimensional window to create a two-dimensional window that is nearly circularly symmetric, by using a process similar to rotation
Creating a rectangular, separable window from two one-dimensional windows, by computing their outer product
The example below uses fwind1 to create an 11-by-11 filter from the desired frequency response Hd. The example uses the Signal Processing Toolbox hamming function to create a one-dimensional window, which fwind1 then extends to a two-dimensional window.
Hd = zeros(11,11); Hd(4:8,4:8) = 1; [f1,f2] = freqspace(11,'meshgrid'); mesh(f1,f2,Hd), axis([-1 1 -1 1 0 1.2]), colormap(jet(64)) h = fwind1(Hd,hamming(11)); figure, freqz2(h,[32 32]), axis([-1 1 -1 1 0 1.2])
Desired Two-Dimensional Frequency Response (left) and Actual Two-Dimensional Frequency Response (right)
The filter design functions fsamp2, fwind1, and fwind2 all create filters based on a desired frequency response magnitude matrix. Frequency response is a mathematical function describing the gain of a filter in response to different input frequencies.
You can create an appropriate desired frequency response matrix using the freqspace function. freqspace returns correct, evenly spaced frequency values for any size response. If you create a desired frequency response matrix using frequency points other than those returned by freqspace, you might get unexpected results, such as nonlinear phase.
For example, to create a circular ideal lowpass frequency response with cutoff at 0.5, use
[f1,f2] = freqspace(25,'meshgrid'); Hd = zeros(25,25); d = sqrt(f1.^2 + f2.^2) < 0.5; Hd(d) = 1; mesh(f1,f2,Hd)
Ideal Circular Lowpass Frequency Response
Note that for this frequency response, the filters produced by fsamp2, fwind1, and fwind2 are real. This result is desirable for most image processing applications. To achieve this in general, the desired frequency response should be symmetric about the frequency origin (f1 = 0, f2 = 0).
The freqz2 function computes the frequency response for a two-dimensional filter. With no output arguments, freqz2 creates a mesh plot of the frequency response. For example, consider this FIR filter,
h =[0.1667 0.6667 0.1667 0.6667 -3.3333 0.6667 0.1667 0.6667 0.1667];
This command computes and displays the 64-by-64 point frequency response of h.
freqz2(h)
Frequency Response of a Two-Dimensional Filter
To obtain the frequency response matrix H and the frequency point vectors f1 and f2, use output arguments
[H,f1,f2] = freqz2(h);
freqz2 normalizes the frequencies f1 and f2 so that the value 1.0 corresponds to half the sampling frequency, or π radians.
For a simple m-by-n response, as shown above, freqz2 uses the two-dimensional fast Fourier transform function fft2. You can also specify vectors of arbitrary frequency points, but in this case freqz2 uses a slower algorithm.
See Fourier Transform for more information about the fast Fourier transform and its application to linear filtering and filter design.