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DIFFRACTION OF SOUND Diffraction around Solid Objects Preliminary note: When a tall, thin sound barrier is interposed between
a point source and a microphone, as shown in Fig., the attenuation provided
by the barrier is theoretically determined by the Fresnel Number, given
by FN = 2ft. Here 'f' is the center frequency of the frequency band used.
't' is the increase in the time that the sound takes to travel over the
barrier over the direct route with no barrier present. Fig. The theoretical relation between insertion loss and FN is shown in Fig.10. Fig.10
Some examples of barrier applications can be tabulated Across the top row are the number of feet from the top of the barrier down to the top of the loudspeaker stack. In the first column is the distance from the loudspeaker stack to the barrier. The listen is presumed to be back in an adjacent community. In each grayed cell is the number of addition feet (d) that the sound must travel.
Example: the top of the barrier is 10 feet above the top of the loudspeaker stack and is 400 feet away. Additional feet is found to be .25. The speaker is a woofer, so use 50 Hz. FN is found be be .025. From the graph the dB reduction is 6. For 500 Hz FN is about 0.22 and the dB reduction is about 9. ***** Copyright 2009 ***** |