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Musical-Applications-of-Microprocessors-2ed-Chamberlin-H-1987

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SOURCE-SIGNAL ANALYSIS 563<br />

o<br />

-5<br />

-10<br />

-15<br />

~ -20<br />

:; -25<br />

Cl<br />

::><br />

!::: -30<br />

-'<br />

c..<br />

~ -35<br />

-40<br />

-45<br />

-50<br />

-55<br />

- 60 '----------'L...Jl""-----,-'-,------'-----L_"'------"------'-'-----"------'JL-J;L---il_l+L-----l1..-.J...........<br />

o 468 624 780 936 1,092 1,248<br />

FREQUENCY (Hz)<br />

(E)<br />

Fig. 16-11. Equivalent half-bandpass filter shapes <strong>of</strong> common windows (cant.).<br />

(E) Hammingwindaws. HM(X) = 0.54 - 0.46 (COS(21TX)), 0 ~ X ~ 1.<br />

Some Example Windows<br />

Now that they can be easily plotted, let's evaluate some windows.<br />

Perhaps the simplest is a linear rise and fall, which is called a triangular<br />

window. This window, along with the upper half <strong>of</strong> its equivalent bandpass<br />

response shape, is plotted in Fig. 16-11B. Two characteristics are immediatelyapparent.<br />

First, the leakage attenuation is much better than that <strong>of</strong> the<br />

rectangular window shown for l'eference. Second, the apparent width <strong>of</strong> the<br />

central lobe, which is the primary bandpass response, is double that <strong>of</strong> the<br />

rectangular window. This is the price that is paid for low leakage, and the<br />

lower the leakage, the broader the bandpass. Thus, one must decide how<br />

much leakage can be tolerated and choose a window that meets but does not<br />

greatly exceed that figure. For our example, a figure <strong>of</strong> -40 dB will be chosen<br />

and none <strong>of</strong> the secondary lobes, even the one closest to the center lobe, will<br />

be allowed to exceed it. According to this criterion, the triangular window is<br />

not suitable, since the first sidelobe is at -27 dB. Nevertheless, the third<br />

and higher sidelobes are less than -40 dB, a figure that seemingly even the<br />

lOath lobe <strong>of</strong> the rectangular window cannot meet.<br />

A similar window is the half sine wave. It has the advantage <strong>of</strong> a flat<br />

rather than pointed top. Its characteristics are shown in Fig. 16-11C. Its<br />

central lobe is only 1. 5 times as wide as the rectangular window, yet has even<br />

better sidelobe attenuation (beyond the first) than the triangular window. Its<br />

second sidelobe, which is at the same frequency as the first triangular window<br />

sidelobe, is about -32 dB.

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