By Douglas Self
All of the layout and improvement concept and path an audio engineer wishes in a single blockbuster e-book! Douglas Self has chosen some of the best sound engineering layout fabric from the Focal and Newnes portfolio and complied it into this quantity. the result's a ebook overlaying the gamut of sound engineering.The fabric has been chosen for its timelessness in addition to for its relevance to modern sound engineering matters. * Hand picked content material, offers every little thing you must understand in a single quantity * confirmed most sensible layout practices * Case histories and layout examples get you off and working in your present undertaking
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The filter response curve is plotted by observing the basilar membrane displacement at the place corresponding to Fc Hz for each input pure tone and plotting this as the filter response at the frequency of the pure tone. This results in the response curve shape illustrated as follows. Fc Fc � (2 * f ) Fc � (4 * f ) Fc � (6 * f ) Fc � (4 * f ) A musical sound can be described by the frequency components which make it up, and an understanding of the application of the critical band mechanism in human hearing in terms of the analysis of the components of musical sounds gives the basis for the study of psychoacoustics.
The first effect is that the ear seems to lump all the energy within a critical band together and treat it as one item of sound. So when all the sound energy is concentrated within a critical band the loudness is proportional to the total intensity of the sound within the critical band. 0 The effect of tone duration on loudness. 0 The effect of tone bandwidth on loudness. 0 100 1000 Bandwidth (Hz) where P1–n the pressures of the n individual frequency components As the ear is sensitive to sound pressures, the sound intensity is proportional to the square of the sound pressures.
How can this be so? The answer is that the sounds are at different frequencies and the sensitivity of our hearing varies as the frequency varies. 12 shows the equal loudness contours for the human ear. These contours, originally measured by Fletcher and Munson (1933) and by others since, represent the relationship between the measured sound pressure level and the perceived loudness of the sound. The curves show how loud a sound must be in terms of the measured sound pressure level to be perceived as being of the same loudness as a 1 kHz tone of a given level.