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Low-pass filter coefficients

FIGURE 4.6 Construction of scaling fnnction (() with low-pass filter coefficients (above). Below the functional representation of the low-pass filter coefficients (left) and their refinement by iterative calculation (increasing resolntion level j) leading to an approximation of the... [Pg.101]

The first row in the wavelet matrix A, simply eontains the low-pass filter coefficients. The second row in the wavelet matrix A, contains the high-pass filter coefficients. As shown above, it is sometimes more convenient to store the filter eoefficients in the matrix A as a sequence of sub-blocks Aj j —. ..,-2,-1,0,1,2,...). The sub-blocks are simply the filter coefficients found in the lattice decomposition and reconstruction equations ar-... [Pg.95]

The Haar low-pass filter coefficients are lo = li = and the respective high-... [Pg.161]

If we let A denote the matrix of filter coefficients with the first row containing the low-pass filter coefficients and the remaining m - 1 rows the sets of high pass filter coefficients and if Nf is the number of filter coefficients contained in each filter, then A will be an m x Nf matrix. A can be partitioned into m x m sub-matrices as follows... [Pg.182]

A solution V to this pair of equations is called a scaling function. It in turn is determined by the numbers (/in), indexed by integers k, which are called (low-pass) filter coefficients. There will be a unique solution v if the following conditions are met [h ] has only finitely many nonzero coefficients, and... [Pg.3217]

Table 1 Coiflet 6 Low-pass Filter Coefficients for the Two-scale Equation... Table 1 Coiflet 6 Low-pass Filter Coefficients for the Two-scale Equation...
The signals were recorded as electrical potential in millivolts. The well known Maxwell s formula and an adjustable empirical coefficients were used to obtain the equivalent volume fraction of liquid [43]. Since it is known that kinematic waves exist only in the frequency of some few Hertz, hardware low pass filter with 20 Hz cutting frequency was included for each channel in the electronic unit. The filter was tuned at 82.66 Db. Data were acquired by a computer at 100 Hz. The following comments regarding the above apparatus description are in order ... [Pg.306]

Figure 3.21 Dattorro s plate reverberator based on an allpass feedback loop, intended for 29.8 kHz sampling rate [Dattorro, 1997]. //i(z)and H2(z) are low-pass filters described in figure 3.11 H (z) controls the bandwidth of signals entering the reverberator, and H2(z) controls the frequency dependent decay. Stereo outputs yL and yR are formed from taps taken from labelled delays as follows yL = a [266] + a[2974] - [1913] + c[1996] - < [1990] - e[187] - f[ 066], yR = < [353] + < [3627] - e[1228] + /[2673] - a[2111] - >[335] - c[121]. In practice, the input is also mixed with each output to achieve a desired reverberation level. The time varying functions u(t) and v(t) are low frequency (= 1 Hz) sinusoids that span 16 samples peak to peak. Typical coefficients values are gj = 0.75, g2 = 0.625, g3 = 0.7, g4= 0.5, g5= 0.9. Figure 3.21 Dattorro s plate reverberator based on an allpass feedback loop, intended for 29.8 kHz sampling rate [Dattorro, 1997]. //i(z)and H2(z) are low-pass filters described in figure 3.11 H (z) controls the bandwidth of signals entering the reverberator, and H2(z) controls the frequency dependent decay. Stereo outputs yL and yR are formed from taps taken from labelled delays as follows yL = a [266] + a[2974] - [1913] + c[1996] - < [1990] - e[187] - f[ 066], yR = < [353] + < [3627] - e[1228] + /[2673] - a[2111] - >[335] - c[121]. In practice, the input is also mixed with each output to achieve a desired reverberation level. The time varying functions u(t) and v(t) are low frequency (= 1 Hz) sinusoids that span 16 samples peak to peak. Typical coefficients values are gj = 0.75, g2 = 0.625, g3 = 0.7, g4= 0.5, g5= 0.9.
Figure 4.4 Similar to the sliding polynomial smoothing (Savitzky Golay filter, the coefficients for 2nd order fit to a parabola) is the effect of Bromba Ziegler filters [Bromba and Ziegler, (1983c), coefficients fit to a triangle upper figure]. Both have bad low pass filter characteristics, as shown in the lower figure with the Fourier transforms of filters through 21 points each. Figure 4.4 Similar to the sliding polynomial smoothing (Savitzky Golay filter, the coefficients for 2nd order fit to a parabola) is the effect of Bromba Ziegler filters [Bromba and Ziegler, (1983c), coefficients fit to a triangle upper figure]. Both have bad low pass filter characteristics, as shown in the lower figure with the Fourier transforms of filters through 21 points each.
Low-pass filter constant Vector of regression coefficients Magnitude of step change... [Pg.334]

In the simplest (and most localized) member of the Daubechies family, the four coefficients [Cq, Cj, C2, C3] represent the low-pass filter H that is applied to the odd rows of the transformation matrix. The even rows perform a different convolution by the coefficients [C3, -C2, Cj, -Cq] that represent the high-pass filter G. H acts as a coarse filter (or approximation filter) emphasizing the slowly changing (low-frequency) features, and G is the detail filter that extracts the rapidly changing (high-frequency) part of the data vector. The combination of the two filters H and G is referred to as a filter bank. [Pg.98]

By iterative application of the FWT to the high-pass filter coefficients, a shape emerges that is an approximation of the wavelet function. The same applies to the iterative convolution of the low-pass filter that produces a shape approximating the scaling function. Figure 4.6 and Figure 4.7 display the construction of the scaling and wavelet functions, respectively ... [Pg.100]

Coarse-filtered (low-pass) wavelet coefficients C(l) of the first resolution level. [Pg.161]

Having the three-dimensional coordinates of atoms in the molecules, we can convert these into Cartesian RDF descriptors of 128 components (B = 100 A ). To simplify the descriptor we can exclude hydrogen atoms, which do not essentially contribute to the skeleton structure. Finally, a wavelet transform can be applied using a Daubechies wavelet with 20 filter coefficients (D20) to compress the descriptor. A low-pass filter on resolution level 1 results in vectors containing 64 components. These descriptors can be encoded in binary format to allow fast comparison during descriptor search. [Pg.182]

The amplifier (5) boosts the signal, eliminates temperature coefficients, and adjusts the offset. The low pass filter (6) limits the bandwidth. The drive circuit is a closed loop system to achieve a stable drive oscillation. It consists of a structure (not drawn) that detects the oscillation movement of the drive of the yaw-rate sensor element, a control unit (2), and an actuator (not drawn). The start circuit (9) initiates the drive oscillation at power on. The block (8) generates all necessary adjustment signals and includes the logic circuit for the trim and an EPROM (erasable programmable read-only memory) for the storage of the trim data. [Pg.302]

For reasons of convenience, and as will be shown in Chapter 6. the decomposition and reconstruction lattice equations can also be written as a pair of equations of recursive matrix products where we separate out the low-pass and high-pass filter coefficients in the form of infinite matrices Cj and Dy. That is. [Pg.97]

Using the notation of Chapter 4, where the low- and high-pass filter coefficients are combined into one matrix, the 3-band DWT outlined in Fig. 1. Going from level 2 to level 1 is written... [Pg.181]


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Filtering low-pass

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